text:
Carol T. Kulik is a Research Professor of Human Resource Management and a senior researcher within the Centre for Workplace Excellence.

Kulik studied industrial-organizational psychology at the University of Illinois at Urbana–Champaign in the United States, and completed a doctorate in business administration, focusing on organizational behavior at the same institution. She taught at UIUC before moving to Arizona State University, then moved to Australia for a position at the University of Melbourne. Kulik later joined the University of South Australia Business School faculty as a research professor of human resource management. Over the course of her career, Kulik has been elected to fellowship of the Society for Industrial and Organizational Psychology, the Academy of Management, and the Academy of the Social Sciences in Australia (2017). She was an associate editor of the Academy of Management Journal and the Journal of Management, and served as the 2018–2019 president of the Academy of Management.

References

Living people
21st-century women scientists
21st-century Australian scientists
Australian psychologists
21st-century psychologists
Australian women social scientists
University of Illinois Urbana-Champaign alumni
Australian women psychologists
University of Illinois Urbana-Champaign faculty
Arizona State University faculty
Organizational psychologists
Academic staff of the University of Melbourne
Academic staff of the University of South Australia
Australian expatriates in the United States
Expatriate academics in the United States
Fellows of the Academy of the Social Sciences in Australia
Academic journal editors
Year of birth missing (living people)

redpajama_set_name: RedPajamaWikipedia


Job Summary Call Receiver provides courteous and professional assistance in responding to member requests for Roadside Assistance for our high volume member service center. We're a mission-driven Member services organization.
We have a saying here at AAA that we aspire to be America's most trusted organization absolutely famous for doing the right thing. With more than four million Members, our purpose is to bring peace of mind to Members so that they can enjoy life more. We work hard to create an environment where you can thrive and where you use your skills and talents to help us deliver legendary Member service.
You will help have a positive impact on the diverse communities we serve. At AAA, there is no clearer directive than to serve our Members and nothing is more important than rescuing our Members in their time of need. Why Work for Us?
Great Pay - $14.50/hour with the opportunity for increases when performance skills blocks are achieved Training – You'll attend a thorough, comprehensive, 6 week training program Benefits – Medical, Dental, Vision, wellness program and more! 401k Matching – $1 for $1 company match up to 6% of pay Annual Incentive Plan – Eligibility to participate in AAA NCNU annual bonus plan Paid Time Off – Ten hours per month, ten holidays annually, one floating holiday and 24 hours per year earmarked for volunteer activities Collaborative Environment – AAA will value your contribution to providing exceptional service to our members Onsite Gym ESSENTIAL FUNCTIONS Call Receiver's provide courteous and professional assistance in response to members requests for Roadside Assistance in a high volume call center. You must properly answer and enter information into the system for each incoming telephone call. On every call you must deliver extraordinary customer service to our Members, using sound business judgment and accurately answering question by applying department policies while using all provided resources.
Accurately enter all information provided by our Members to ensure proper service is rendered. Set proper expectations with our Members to ensure their complete understanding of the services they will be given. Demonstrate empathy when dealing with Members in high stress situations.
Ensure Members are fully aware of products available to them to enhance the Member's experience for each and every Member's individual situation. (upgrading coverage, etc.) KNOWLEDGE/SKILLS/ABILITIES Clear verbal and written communication Data entry skills, typing (35 wpm minimum), computer, telephone and basic math Passion for customer service Ability to use a navigation system (Google maps, iOS Maps, Waze… etc.) Ability to work weekends and holidays as necessitated by business and/or weather conditions Ability to cope in a professional manner with a fast work pace and time pressure EDUCATION & EXPERIENCE / LICENSES & CERTIFICATION High School diploma or equivalent required – college education credits preferred 0 – 2 years prior customer service experience is preferred We'll value your skills and experience. We're building a performance organization with heart and developing a pipeline of tomorrow's leaders. Your work will be enhanced with training opportunities, a mentoring program and our promote-from-within philosophy.
We celebrate our diversity and leverage the power of many minds. ABOUT US For over a century, AAA has continued to redefine itself to become a multi-faceted leading provider of travel, insurance and auto services. We know you're as versatile as we are and that every aspect of your personality adds to the skills and knowledge you bring to AAA.
Datrose is seeking an experienced Sr. Network Controller (O&M NOC) with Secret Clearance for an excellent Long-term Temporary Assignment at Hill AFB, UT! If interested in exploring, please apply directly at www.datrose.com/careers.
Note: Must be a US Citizen.
Responsible for overall network engineering support for customer programs including planning, designing, and evaluating various components of the Defense Information Systems Agency (DISA) Enterprise Network.
Able to work in a rotating shift work environment as we are a 24/7 operation.
Experience with one or more of the following: alarm surveillance, fault management, WAN maintenance, performance management.
Note: An IAT Level II certification (GSEC, Security+ CE, SSCP, or CCNA Security) is required.
However, we will hire someone without one of these certifications---provided candidate can obtain an approved baseline certification within 90 days of start date. Those hired who fail to obtain one of these certifications within the 90-day grace period will be terminated.
Datrose is seeking an experienced Network Engineer for an excellent temporary assignment (W2 Only) opportunity in Hill AFB, Utah. This is an excellent opportunity for the right individual. If interested in exploring this great opportunity, please apply directly atwww.datrose.com/careers. PRIMARY RESPONSIBILITIES: * Responsible for overall network engineering support for customer programs including planning, designing, and evaluating various components of the DISA Enterprise Network.
Experience with one or more of the following: alarm surveillance, fault management, LAN maintenance, performance management *Able to work in a shift work environment as we are a 24/7 operation.


"Enable SNMP on Windows Server 2003/2003R2"
"Change Alert Center Threshold Description"
If you have a problem with WhatsUp Gold database size, you can use Database Tools to Purge expired rows. But if you have non expired data and you need to delete, so you should delete them directly from database.
Tables that have an unexpectedly large number of rows in them may indicate a problem. You can either DELETE or TRUNCATE the table. DELETE option is a more measured approach, whereas the TRUNCATE option empties the table. For DELETE you can do so in small chunks, by date; however, this process will be slower.
If the Statistical tables are the ones that happen to be large, then choose to either DELETE or TRUNCATE.
You have made a backup before performing Delete or Truncate.
You can change the time to the required one.
Make sure that if you are collecting SNMP Traps or Syslogs, that "Accept Unsolicited" is not enabled under the Passive Monitor Listeners (WhatsUp Gold Server Console > Configure > Program Options > Passive Monitor Listeners).


text:
Микола Уварович Котлюба (, село Благовіщенка, тепер Кам'янсько-Дніпровського району Запорізької області — , місто Кам'янка-Дніпровська Кам'янсько-Дніпровського району Запорізької області) — український радянський діяч, секретар парткому виробничого об'єднання «Запоріжтрансформатор» імені Леніна Запорізької області, 1-й секретар Ленінського райкому КПУ міста Запоріжжя. Член ЦК КПУ в 1981—1990 роках.

Біографія
У вересні 1948 — червні 1958 року — учень Благовіщенської середньої школи № 1 Кам'янсько-Дніпровського району Запорізької області.

У вересні 1958 — березні 1959 року — учень комутатника цеху КРУ, у березні 1959 — серпні 1960 року — слюсар-електромонтажник цеху КРУ Запорізького трансформаторного заводу.

У вересні 1960 — березні 1964 року — студент Запорізького машинобудівного інституту. У березні 1964 — лютому 1965 року — інженер-конструктор відділу головного конструктора Запорізького трансформаторного заводу. У лютому — серпні 1965 року — студент Запорізького машинобудівного інституту, інженер-електромеханік.

У серпні 1965 — березні 1970 року — інженер-конструктор відділу головного конструктора Запорізького трансформаторного заводу. У березні 1970 — жовтні 1975 року — керівник групи відділу головного конструктора, начальник відділу технічного контролю Запорізького трансформаторного заводу.

Член КПРС з квітня 1970 року.

25 жовтня 1975 — 20 листопада 1986 року — секретар партійного комітету КПУ виробничого об'єднання «Запоріжтрансформатор» імені Леніна міста Запоріжжя. З 1979 по 1982 рік навчався на заочному відділенні Вищої партійної школи при ЦК КПУ.

20 листопада 1986 — 24 квітня 1991 року — 1-й секретар Ленінського районного комітету КПУ міста Запоріжжя.

У квітні — червні 1991 року — генеральний директор науково-виробничого об'єднання «Трансформатор» у Запоріжжі. У червні 1991 — березні 1997 року — президент — генеральний директор підрозділу «Техноком» Запорізького заводу високовольтної апаратури.

У березні 1997 — 18 жовтня 1998 року — 1-й заступник голови Кам'янсько-Дніпровської районної державної адміністрації Запорізької області.

Нагороди
 орден Трудового Червоного Прапора
 орден Дружби народів
 медалі

Джерела
 газета «Запорізька правда» (Запоріжжя) — січень 1981 року.

Керівники підприємств Запоріжжя
Персоналії за алфавітом
Члени КПРС
Випускники Запорізького національного технічного університету


When Specter learned that Graham, with the Administration's support, was trying to ban the detainees from filing more habeas cases, he did everything he could as chairman of the Judiciary Committee to stop the idea, including filing an amendment to the bill. With just a few days' notice, he convened a hearing on the plan to strip the courts of jurisdiction in the detainees' cases. The session took place on September 25th, a Monday morning, a time rarely devoted to Senate business.
Two days after the hearing by the Judiciary Committee, debate began in the Senate on Specter's amendment to preserve the right of detainees to bring habeas cases. "The right of habeas corpus was established in the Magna Carta in 1215, when, in England, there was action taken against King John to establish a procedure to prevent illegal detention," Specter said. "What the bill seeks to do is set back basic rights by some nine hundred years." As several of his Republican colleagues, including Graham, Cornyn, and John Kyl, of Arizona, rose to support the habeas ban, Specter deftly parried their arguments, without consulting aides or notes.


text:
Journal of Midwifery & Women's Health
The Use of Herbs and Dietary Supplements in Gynecology: An Evidence-Based Review
Cathi E. Dennehy, PharmD
J Midwifery Womens Health. 2006;51(6):402-409.
Abstract and Introduction
Consumers frequently use herbs and dietary supplements to treat chronic conditions that are poorly responsive to prescription drugs or when prescription drugs carry a high side effect burden. Women may use herbs and supplements for chronic gynecologic conditions, such as menopause, premenstrual syndrome, dysmenorrhea, cyclic mastalgia, and infertility. This review is an evidence-based evaluation of herbs and supplements for these conditions. Therapies that carry a higher level of support from randomized controlled trial evidence include black cohosh for menopause; vitamins B1 and E for dysmenorrhea; calcium, vitamin B6, and chasteberry for premenstrual syndrome; and chasteberry for cyclic mastalgia. There were too few trials involving herbs and supplements in infertility to warrant a solid recommendation, but chasteberry, antioxidants, and Fertility Blend have some preliminary support. Midwives may want to consider these alternatives in addition to more traditional treatment options when meeting with patients.
Sales of dietary supplements in the United States rose from $15.7 billion in 2000 to $18.7 billion in 2002.[1] According to a recent telephone survey of 8470 Americans, the use of herbs and other natural products, excluding vitamins and minerals, increased from 14.2% in 1998 to 1999 to 18.8% in 2002.[2] Product users were more likely to be women, of white ethnicity, who have high levels of education and income.[2] In general, herbs and supplements appeal to Americans because they are perceived as being natural with fewer side effects than prescription and over-the-counter medicines.[1] Consumers believe that these products may help them to live longer and will generally improve overall health and well-being.[1] These supplements are frequently used to treat chronic medical illnesses in which therapeutic options are limited, costly, or carry a high side effect profile.[1] Women experiencing symptoms of menopause, premenstrual syndrome, dysmenorrhea, mastalgia, and infertility may seek alternative therapies and medical providers who are open to using them.
Certified nurse-midwives and certified midwives (CNMs/CMs) are likely to assist women in the management of gynecologic conditions that extend beyond pregnancy. The use of herbs in pregnancy is common among nurse-midwives. In a national survey, 52% of respondents used herbs for cervical ripening and induction or augmentation of labor.[3] It is likely that herbs and supplements may also be employed in the management of gynecologic conditions.
Dietary supplements are currently governed by the Food and Drug Administration under the Dietary Supplement Health and Education Act. The act defines a supplement as "a product (other than tobacco) intended to supplement the diet that bears or contains one or more of the following: a vitamin, mineral, herb or other botanical, amino acid, a dietary substance used by man to supplement the diet by increasing the total dietary intake or a concentrate, metabolite, constituent, extract or combination of any of the ingredients described above."[1] Dietary supplements are regulated as foods and can be marketed to consumers without providing support for claims of efficacy and safety. The Food and Drug Administration has limited authority over these supplements and can only remove a product from the market if it can show proof of posing "an unreasonable risk of injury or illness" to consumers through postmarketing surveillance.[1] Health care providers who use dietary supplements in their practice should be aware of these limitations.
Some herbs may be discussed below with reference to the recommendations of the German Commission E.[4] The Commission is a group of German researchers, who in conjunction with members of industry, compiled recommendations regarding the safety and efficacy of more than 300 herbal products. Herbs were "approved" for certain indications if they showed reasonable proof of efficacy and safety. However, "approval" for a certain indication does not necessarily imply evidence from randomized controlled trials (RCTs).
This article takes an evidence-based approach in reviewing the use of herbs and dietary supplements for management of symptoms associated with menopause, dysmenorrhea, PMS, mastalgia, and infertility.
J Midwifery Womens Health. 2006;51(6):402-409. © 2006 Elsevier Science, Inc.
Cathi E. Dennehy, PharmD, is Associate Clinical Professor, School of Pharmacy, UCSF, San Francisco, California.
The author does not have any commercial affiliation that would affect the integrity of this manuscript.
Article 5 Things to Know About Alternative Therapies and Cancer
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b:recommendationscuratedHasData : false

redpajama_set_name: RedPajamaCommonCrawl


text:
Q: Create comparable dice format from 2d array? So I have this problem that I want to make a 2d array to a dice format I can compare.
So if the 2d array is for example:
00100
02340
00500
00600
(0 = blank space)
would be:
image
So if you fold it in you get a dice. My problem is I need it in a format so I can compare if it's different from another dice.
For example:
00600
00500
04320
00100
Is the same as the other example, so I need it in a format where I can compare them. The rotation of numbers doesn't matter. Any ideas?

redpajama_set_name: RedPajamaStackExchange


At last! Wood stain suitable for use with wood-epoxy composite boats. Click here for Nick Schade's tips on getting the most out of Behlen's Solar-Lux Stain.
Solar-Lux Stain is a highly fade- and UV-resistant dye base non-grain raising stain. The deep penetration and colorful transparency brings out the natural beauty of the wood. Solar Lux stains may be intermixed to achieve customized shades. It dries in approximately one hour and may be overcoated with epoxy.
H. Behlen & Bro.'s wood finishing products come from a 110-year tradition of quality and expertise. Founded in 1888 by a German-born chemist, the firm was the first to offer finishing products used by European master craftsmen in the American market. Behlen's extensive knowledge of furniture making and finishing has been behind the development of every product, and has made the company an acknowledged leader in its field.
* International Customers: we do not ship this product overseas.
A must for a fine edge.
Staining a Wood Strip Kayak - a video shop tip courtesy of Nick Schade.


1918 House Bill 0078. Resolve Providing For The Construction Of A Fireproof Vault At The Rutland State Sanatorium.
Title 1918 House Bill 0078. Resolve Providing For The Construction Of A Fireproof Vault At The Rutland State Sanatorium.


text:
Station Owner's Finances and Alleged Suicide Attempt Make Boston Headlines
Station Owner's Finances and Alleged Suicide Attempt Make Boston Headlines
The Boston Herald reported a suicide attempt by WBIX(AM) owner Bradford Bleidt, saying he first delivered a taped confession to the Securities & Exchange Commission detailing how he allegedly stole a fortune from clients of his financial planning firm.
He was reported by the newspaper to be in critical condition.
The paper also stated that the development has raised questions about the future of the all-business station and "has left staffers wondering who, if anyone, will pay their salaries."
Bleidt reportedly purchased a controlling interest in the station earlier this year.
"Hello, my name is Brad," the tape began, "and I'm reporting a serious breach of professional conduct and just criminal behavior. I'm reporting myself." The tape went on to state that Bleidt "over the last twenty years" had "stolen tens of millions of dollars from clients through Allocation Plus." According to transcripts, some of the funds were used to acquire a controlling stake in WBIX, and possibly to subsidize the station's operations.
Thursday, Nov. 11 is the day Bleidt termed his "day of reckoning," as there was a client that needed "a million-and-a-half dollars wired into their account that's supposed to be there this morning. Obviously, it's not going to be there this morning because the money is gone," the transcript reads.
The Herald reported that emergency action was taken last Friday in U.S. District Court, when the SEC froze Bleidt's personal assets and the assets of his company. The Securities Division of Secretary of State William F. Galvin's office took similar actions, authorities said. Additionally, the court appointed a receiver for Allocation Plus, while issuing a temporary restraining order to prevent further violations of the SEC's anti-fraud rules.
"All we really know is what he confessed to," said Silvestre Fontes, senior trial counsel for the SEC. "Millions of dollars were stolen over the last 20 years." He added that SEC investigators had questioned employees and examined documents on Friday at Allocation Plus' offices.
Details of how Bleidt injured himself could not be corroborated by the newspaper.


text:
Japan's real estate becomes greener
Continuity in addressing the sustainability topics will further support the development of a resilient real estate market in Japan.
Naoko Iwanaga
Japan was classified amongst the transparent real estate markets in 2012 when JLL had started surveying factors relating to sustainability in the Global Real Estate Transparency Index (GRETI) − one of our flagship reports generated biennially. Over the years, sustainability initiatives became more mainstream with intensive efforts by public and private sectors to support the occupational and investment real estate markets. Starting with GRETI 2020, JLL included net zero carbon, resilience and wellness as components of the sustainability subindex. Japan continued to rank amongst the top-performing countries but still has room for improvement
Figure 1: Image of Future Development
Japan is no exception to the widespread adoption of Green Building certification and energy efficiency standards that is observed worldwide.
The Comprehensive Assessment System for Built Environment Efficiency (CASBEE) is a government initiative developed by the Institute for Building Environment and Energy Conservation (IBEC) to evaluate the environmental sustainability performance of new and existing buildings. The number of buildings certified by the first-class architects (qualified as evaluators by IBEC) has approached close to 1,000 as of April 2020.
The Act on Improvement of Energy Consumption Performance of Buildings, implemented in April 2016, aims to further decrease carbon emissions. More mid-sized office buildings will need to conform to the standards after revisions was announced in September 2020 and to be enforced in April 2021. The new standard sets the minimum non-housing floor area at 300 square metres, down from 2,000 square metres.
On the other hand, the adoption of a green building performance benchmark (like for most of the world) awaits implementation despite the need by domestic and international investors who recognise sustainability as an essential component for a resilient building.
The occupational market has seen the adoption of green leases increase, particularly amongst buildings owned by J-REITs, yet its representation to the total is small and only voluntary. In addition, there is room for improvement for the newly added factors of net zero carbon, resilience and wellness frameworks.
The government has set ambitious targets relating to net zero energy buildings (ZEB) for newly constructed buildings to adopt self-explanatory designs. The deadline for public buildings was 2020, and 2030 for public and private buildings. Though the target has the provision of guidelines and subsidy offerings, it remains voluntary to date. CASBEE has designed a resilience residence checklist drawing attention to a healthy dwelling and risk recognition, but it has yet to be standardised.
Finally, CASBEE's Wellness Office Certificate, which assesses buildings and workplaces from the viewpoint of workers' health, workplace productivity and resilience, appears to be a genuine government oversight programme available to the public. However, the number of certified buildings is small (30 as of February 2021) due to its relatively recent launch, indicating the need for wider adoption.
The acknowledgement of sustainability as a key component for a better tomorrow has been gaining traction for some time. The pandemic has accelerated this trend by changing people's values and lifestyles across the world. Policy continuity and achieving the above mentioned objectives will further promote a sustainable and resilient real estate market in Japan.
The changing role of supermarkets in Australia
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Call for Energy Assessment during Construction stage - India


JD Wetherspoon has announced the disposal of 20 town and city centre public houses. The portfolio comprises of 15 freehold properties and five leaseholds. The properties are available individually, as a small package or as an entire portfolio.
The Restaurant Group Plc has announced plans to dispose of a further 22 restaurants. Spread across England, Wales and Scotland, the properties are available individually and are located in shopping centres, retail parks and also roadside locations.
Punch has acquired four pubs from Mitchell's of Lancaster: Th'Owd Tithe Barn in Garstang, The William Mitchell in Morecambe, Royal Oak in Bolton on Sands as well as The Duke of Rothesay. Pub and Bar Magazine reports that Mitchell's of Lancaster, originally founded in 1871, fell into administration in 2018.
Arc Inspirations has opened Banyan Bar & Kitchen in Newcastle, marking their first operation in the city and the ninth Banyan to open in the north of England. Pub and Bar Magazine reports that the 10,000 sq ft site, previously occupied by Jamie's Italian, has undergone a £1.5m refurbishment.
Preet Tandi, the chef behind the Soho Wala Indian street food restaurant in Soho's Courthouse hotel, is opening Colchester Kitchen, a Japanese-Mexican fusion restaurant, at the 16-bedroom Essex hotel Prested Hall. The Caterer reports that the 80-cover restaurant is due to open in August.
BrewDog, the Scottish brewer and retailer, has announced intentions to open a DogHouse hotel in the London. The Morning Advertiser reports that the 'craft beer hotel' concept launched in Columbus, Ohio in the US.


text:
\section{CRYSTAL GROWTH AND EXPERIMENTAL METHODS}

\subsection{Crystal growth and characterisation.}

Single crystals were grown in sealed quartz tubes, using the reaction PdCl$_{2}$ + 2CoO $\rightarrow$ PdCoO$_{2}$ + CoCl$_{2}$, and extracted in hot ethanol.  We broadly followed procedures described in Ref.~\textit{(17)} , but experimented with modified temperature profiles to optimize the growth.  Standard x-ray diffraction, chemical analyses and transport measurements were used for initial characterization of the phase purity and high conductivity of the crystals.

\subsection{Calculating resistivity and the momentum-relaxing mean free path. }

In a rectangular parallelepiped with homogeneous current flow, the resistivity ρ is deduced from measured resistance using the formula $\rho$ = $RLW/T$, where $R$ is the measured resistance, $L$ the spacing between the voltage contacts, $W$ the width and $T$ the physical thickness of the sample.  In a highly two-dimensional material such as PdCoO$_{2}$, whose in-plane conductivity is a thousand times larger than that between the planes, the effective electrical thickness $T_e$ can differ from $T$: if the voltage contacts are not far enough from the current injection point, the current has not spread through the entire thickness of the crystal before passing between the voltage contacts.  In bulk measurements this issue is typically avoided by attaching current leads over the end faces of the sample in an attempt to inject the current evenly across the whole thickness. In this work, however, the sample and contact geometries involved current injection through the top surface.  Calculation for a parallelepiped modeled on the device shown in Fig.~1A  showed that a modest difference between $T$ and $T_e$ was likely.  The main resistivity results are normalized in such a way that any correction factor between $T$ and $T_e$ would drop out from the $\rho/\rho_{0}$ axes of Fig.~4, but the factor is important to accurate determination of the momentum-relaxing mean free path $\ell_{MR}$.  Rather than rely quantitatively on such a calculation, which would inevitably involve some assumptions, we fabricated the extra device shown in Fig.~S1, from a crystal of similar thickness to that shown in Fig.~1 A.  By studying the evolution of the measured $\rho$ along the length of this multi-contact device, we determined that, for a device with the geometry shown in Fig.~1 A, $T_e$ =$ \alpha T$, with $\alpha$ = 0.75 $\pm$ 0.05.  Analysis of our channel data using $\alpha$ = 0.75 and allowed determination of $\rho_0$ = 8.5 $\pm$ 0.6 n$\Omega$cm. This is in excellent agreement with other measurements on bulk crystals from the same batch.

The error associated with converting the measured resistivity $\rho_0$ to the bulk mean free path is lower than that in determining $\rho_0$.  In a two-dimensional metal, the resistivity is given by the line integral of the mean free path $\ell$ around the Fermi ``surface''.  At the low temperatures relevant to the data shown in Figs. 2~-~4, $\ell$ can be assumed to be independent of k in the isotropic-$\ell$ approximation~\textit{(33)} but in P\lowercase{d}C\lowercase{o}O$_{\text2}$ this is a very mild approximation since the Fermi velocity v$_F$ is almost k-independent in any case.  If the Fermi surface has circular cross-section we arrive at the famous two-dimensional expression $\ell$ = $\frac{\textit{hd}}{{\textit{e}^2\textit{k}_F\rho}}$, where $\textit{k}_F$ is the Fermi wave vector and $\textit{d}$ is the interlayer spacing.

If the Fermi surface is not circular, a correction is required to this formula because, for a given area, the perimeter around which the line integral is performed is longer than that of a circle. The correction is usually small for the shape close to a circle. For the rounded hexagonal Fermi surface of PdCoO$_2$ ~\textit{(16, 25)}  it is straightforward to estimate it numerically, and it produces a 2$\%$ change in the calculated mean free path from that estimated by simply using Eq. S1 and k$_F$ defined as $(A/\pi)^{1/2}$ where the Fermi surface area $A$ is known to within 1$\%$ accuracy from the quantum oscillation frequencies. The perimeter change was taken into account in our calculation.  Taking into account the uncertainty in $A$, and combining with that in $\rho_0$ yields $\ell_{MR}$ = 18.5 $\pm$ 1.5$\mu m$.

After completing our channel narrowing experiments, we verified the validity of our two-dimensional approximation by etching the narrowest channel from above, to reduce its thickness.  Measurements before and after this step showed the expected change in resistance but no change in resistivity, as expected for a two-dimensional material.

\subsection{Focused Ion Beam sample fabrication}

Using Focused Ion Beam (FIB) fabrication to study the width dependence of the resistance of micro-channels is a relatively new approach and thus special care must be taken to investigate potential issues arising from this technique. In particular, the nature of defect generation due to the 30kV ion irradiation in the crystal bulk as well as the sidewalls of the microwires need to be considered. In the following, we will discuss the fabrication details and the expected state of the sidewall surfaces. For a general introduction into the details of FIB micromachining, we refer to ~\textsl{(34)}  and~\textsl{(35)}.

{\bf FIB fabrication:} The PdCoO$_{2}$ crystals grow naturally as thin platelets, with a typical in-plane width in the few 100 $\mu$m range and a typical thickness around 10 $\mu$m. Crystals were first screened under an optical microscope for evident macroscopic defects such as strong terrace growth, cracks and intergrowths. Platelets with clear hexagonal morphology and immaculate surfaces were chosen for further fabrication. The crystals were glued with epoxy onto a silicon chip and sputter-coated with 150 nm of gold. This gold was structured by FIB milling into the desired contact configuration. A Helios Nano Lab 600i by FEI was used for the sample preparation.

In a following step, the crystals were coarsely structured into their final geometry. FIB milling is a fairly gentle way of structuring compared to mechanical abrasion, laser or spark-erosion, and as a result, it is a slow process. Therefore coarse structuring was performed at a high ion flux (25-40~nA). It is important to note that high ion flux cutting does not generate more defects: Higher currents are achieved by using broader beams, so that the flux density of ions impacting on the sample remains low. Further, the beam is purposely defocused to spread out power over an even bigger beam spot. Cutting a crystal into the shape shown in Fig.~1 takes about 12h.

The broad beam spot used for coarse cutting leads to rough and rounded edges. Therefore it is essential to polish the sidewalls. The polishing procedure involves cutting the last micron using smaller currents with smaller spot sizes. Three currents of 2.5~nA, 780~pA and 320~pA were used successively as the sidewall approached the final desired thickness.

{ \bf Width determination:} The presented results critically rely on a precise determination of the effective width of the sample. The milling process will always create slightly canted sidewalls. After an initial rounding on the top, basically vertical sidewalls were achieved. The effective width was then calculated by taking the average as (2 $W_{bottom}$+$W_{top}$)/3. This weighted average takes the initial rounding of the edges at the top into account. An example measurement using Scanning Electron Microscope (SEM) images is given in Figure S2. Most importantly, the same methodology was used throughout the study to ensure consistent determinations of the sample width.

{\bf Surface damage:} Another important aspect concerns the nature and depth of the ion beam induced surface damage layer. While the strong Shubnikov-de Haas oscillations observed in our patterned samples clearly evidence the high crystal quality of the bulk, a surface damage layer of a priori unknown extent surrounds the pristine core. To estimate the effective thickness of the amorphous layer, we performed a full damage cascade Monte Carlo simulation using the widely used software SRIM (Stopping and Range of Ions in Matter) ~\textit{(36)}.

Fig. S3 shows the depth profile of 30kV Ga ions impacting on the surface under realistic conditions of quasi-grazing incidence. The typical implantation profile follows a Gaussian distribution centered around the lateral stopping range, which is around 2~nm at this high incidence angle. The Ga implantation is suppressed exponentially by simple statistical arguments of a random walk by one decade every 6nm up to 20~nm, where a sudden drop in ion penetration signals a cut-off. At the same time, inelastic processes due to the ion-matter interaction generate phonons as well as defect cascades. These phenomena generally follow the profile of the implantation, which an integration over the inelastic processes in the simulation confirms. Therefore we estimate the damage layer to be on the order of 20~nm at each boundary in PdCoO$_2$.  We note that the relatively large atomic number of Pd is advantageous in reducing the ion implantation lengths.  SRIM calculations have been confirmed to accurately capture the Ga penetration during the FIB process, for example via atom probe tomography~\textit{(37)}, which also confirms the random nature of ion implantation.  This in turn ensures that the edges are rough from the point of view of electron boundary scattering.  This rough wall approximation is therefore adopted in our boundary scattering calculations. Combining the slight edge damage with our estimate of small lateral width variations after final polishing, we believe that a conservative estimate of the total error in our determination of width is 80 nm or less.  This would be approximately a 10$\%$ effect in our narrowest channel, falling successively for larger widths.

A check both on our width determination procedure and the overall width uncertainty is to compare the width obtained from the procedure outlined above with that deduced from magnetoresistance.  As discussed in the main manuscript and shown in Fig.~2, we observe well-defined maxima in the magnetoresistance for all studied widths.  The appearance of these maxima is a well-known phenomenon observed in very clean metals confined into structures smaller than the mean free path. The existence of a well-defined maximum evidences that a reasonably well-defined ``effective width" exists (a triangular cross-section would not result in such a maximum).  Further, the field values of the maxima for channel widths greater than 2 $\mu$m follow the relationship $\textit{B}_{max} = 0.62\frac{\hbar\textit{k}_F}{\textit{We}}$  to high accuracy.  If, instead of relying on the width measurements, we use the measured field maxima to deduce the widths of our narrowest channels, we see excellent agreement between the two methods: 0.73 $\mu$m (SEM measurement) cf 0.79 $\mu$m (magnetoresistance peak);  1.17~$\mu$m (SEM measurement) cf 1.15~$\mu$m (magnetoresistance peak);  1.90~$\mu$m (SEM measurement) cf 2.09~$\mu$m (magnetoresistance peak).  This gives us further confidence both in the method we have used to deduce the width from SEM images and in our error estimates.

\subsection{Checks for length dependence and possible internal heating. }

When studying transport properties on short length scales, there is the possibility of creating significant Joule heating resulting in both a raised average electronic temperature and a temperature distribution across the sample leading to a position-dependent resistivity.  If these effects were very large, they might also lead to non-linear I-V characteristics, especially in the presence of phonon drag.  We verified during our main experiment that we resolved no I-V non-linearity, but since this would be a second-order effect, that does not necessarily rule out significant average sample heating.

Before discussing explicit tests of the electronic temperature and its distribution, we note that a large effect is unlikely.  Although current-dependent heating is an issue in samples with high resistances, our experiments are performed on an extremely good metal with a carrier concentration a factor 10$^4$ higher than those in the semiconductor devices studied in the beautiful work of the 1990s~\textit{(3, 4)} .  Further, we have approximately 16000 layers in parallel when we work at our standard constant r.m.s. measurement current of 10~mA, 177~Hz (corresponding to voltages in the range 200~nV to 2~mV r.m.s depending on the device dimensions).  For the narrowest channel we reduced this to 8000 layers in parallel, but worked at 1~mA r.m.s current.  This means that we are applying a maximum of just over 0.5~$\mu$A r.m.s. per layer.  Typical power dissipation in our devices is in the range nano- to microwatts, several orders of magnitude lower than the cooling power of the $^4$He cryostat used for the measurements, and the sample is thermally anchored to the external thermal reservoir through high conductivity metallic current and voltage leads and through direct epoxy contact along its length.
That these methods of thermal sinking are effective can be seen in several ways.  Firstly, we observed high resolution quantum oscillations in the resistivity when working at a reservoir temperature of 1.9~K.  The oscillations have a strong intrinsic temperature dependence when observed in equilibrium magnetic measurements ~\textit{(18)}, and the spectrum we saw (Fig.~3C) would not have been observable if the average electron temperature had been even one degree higher.  Further, we saw no change to the relative weighting of the frequencies as the power dissipation in the device changed by over a factor of two during the experiment.  Both of these observations are consistent with the electronic temperature being very close to that of the reservoir at our measurement currents.
Further checks on this come from the length dependence of the measured resistances, which scaled linearly with length in all studied devices, even up to the largest meandered device used for the quantum oscillation experiments (Fig.~1B). With a total length of 4600~$\mu$m, this is the largest structure we studied. The thickness of crystals of this macroscopic size is never homogeneous over such large distances, and indeed we observe steps in the thickness (Fig.~1B). Nonetheless we can calculate the average dimensions of the device: Length 4600~$\mu$m, thickness 17.1~$\mu$m, width 6~$\mu$m. In zero applied field, this device has a 4-terminal resistance of 9~m$\Omega$ at 2~K, and using these average dimensions we obtain a resistivity of 20~n$\Omega$ cm. We conservatively estimate an error of about 15\% for the uncertainties in the geometry. In spite of being 46 times longer than the device used for the channel narrowing experiment, the two resistivities agree for $\it{W}$ = 6~$\mu$m to within experimental error.
To perform a still more precise check for length scaling of the resistance within the same crystal, and also to check for the influence of the length of the current path, we fabricated the device shown in Fig.~S4.  The deviations in resistivity between the accessible equally spaced voltage leads (50~$\mu$m spacing) scales with length as expected within an experimental uncertainty of 2\%. For example, sourcing a current through the main structure (colored purple in Fig.~S1) at 2~K, we measure a resistance R$_{12}$ = 89.7~m$\Omega$ between the contacts V$_{1}$ and V$_{2}$; and R$_{13}$ = 177.9~m$\Omega$  between V$_{1}$ and V$_{3}$. The ratio R$_{13}$ / R$_{12}$ = 1.983 agrees well with the ratio of the device length, L$_{13}$ / L$_{12}$ = 100~$\mu$m / 50~$\mu$m = 2 as expected for the usual linear dependence of resistance to conductor length.

In this structure, we can also directly check for influence of the current path length. The total length of the conductor between the main current pads is 2700~$\mu$m  (purple). By injecting the current alternatively through the contacts V$_{1}$ and V$_{4}$, the effective length of the current path is reduced by more than a factor of 3 to 840~$\mu$m . The resistance R$_{23}$ measured between the central voltage contacts V$_{2}$ and V$_{3}$ e is the same within 2\% accuracy for both current cases (89.7~m$\Omega$  at 2700~$\mu$m  conductor length, 91.2~m$\Omega$ at 840~$\mu$m  conductor length).

Taken together, we believe that these checks rule out a significant influence of Joule heating or other sources of systematic error leading to length-dependent resistivity in our experiments.

\section{Hydrodynamic electrons: theory}

We first shall give an overview of the theoretical description of
the electrons as a two-dimensional hydrodynamic fluid of charged
particles obeying Fermi statistics.  We assume that the scattering of
the electrons is comprised of three components, namely
momentum-relaxing collisions with impurities and wire boundaries and
momentum-conserving electron-electron scattering.  In particular we
ignore electron-phonon interactions as well as electron-electron
umklapp scattering processes.  Our calculation closely follows the
beautiful work of de Jong and Molenkamp~\textit{(4)} and
reproduces their result.  Secondly we illustrate a simple hydrodynamic
model describing the electrons as a flow of classical charged
particles characterized by their viscosity.

\subsection{Momentum conserving and momentum relaxing scattering}
\label{sec:dejong}

Following Ref.~\textit{(4)}, we start with a semiclassical
description of the motion of the electrons, and use the standard
Boltzmann transport equation
\begin{equation}
    \frac{{\rm d}f}{{\rm d}t}=
    \frac{\partial f}{\partial t}
    +
    \sum_{i}\left(
    \frac{\partial x_{i}}{\partial t}
    \frac{\partial f}{\partial x_{i}}
    +
    \frac{\partial v_{i}}{\partial t}
    \frac{\partial f}{\partial v_{i}}
    \right)
    =
    \left.\frac{\partial f}{\partial t}\right|_{\text{imp}}
    \label{eqn:boltzmanntransport}
\end{equation}
for the distribution function $f(\vec x,\vec v)$ in the phase space of
the electrons at positions $\vec x=(x_{1},x_{2})^{T}$ with velocity
$\vec v=(v_{1},v_{2})^{T}$ in a two-dimensional wire.  The term on the
right-hand side of the equation denotes the momentum relaxing
collisions of the electrons violating Liouville's theorem.

The electrons with mass $m$ are subject to a Lorentz force $\vec
F=\hbar(\partial\vec k/\partial t)=m(\partial\vec v/\partial t)=-e\vec
E$ in the applied static electric field, thus we can replace
Eq.~(\ref{eqn:boltzmanntransport}) with
\begin{equation}
    \sum_{i}\left(
    v_{i}\frac{\partial f}{\partial x_{i}}
    -\frac e\hbar E_{i}\frac{\partial f}{\partial k_{i}}
    \right)
    =
    \left.\frac{\partial f}{\partial t}\right|_{\text{scatt}},
    \label{eqn:boltzmann}
\end{equation}
where we define $(\partial f/\partial t)_{\text{scatt}}$
to formally comprise all remaining contributions to $f$.

At equilibrium, $f$ is given by the Fermi-Dirac distribution
$f_{0}=\left[\exp\left(\beta(\epsilon-\mu)\right)+1\right]^{-1}$ with
single-particle energies $\epsilon=\hbar^{2}/(2m)\vec k^{2}=(m/2)\vec
v^{2}$ and Fermi energy $\mu$.  The temperature of the electrons in
the wire is $T=(k_{\text B}\beta)^{-1}$.  At small electric fields
applied in $x_{1}$ direction along the wire, we can expand around
the equilibrium,
\begin{equation}
    f(\vec x,\vec v)=f_{0}+
    \left(-\frac{\partial f_{0}}{\partial\epsilon}\right)
    \chi(x_{2},\phi),
    \label{eqn:lb}
\end{equation}
which implies that the nonequilibrium part of the distribution
function in momentum space is only in a small area around the
(circular) equilibrium Fermi surface.  Spatially $f(\vec x,\vec v)$
only depends on the transverse coordinate $x_{2}$, and its velocity
dependence, writing $\vec v=v\hat v$ with $\hat
v:=(\cos\phi,\sin\phi)^{T}$, is split into an energy dependent part
given by $(\partial f_{0}/\partial\epsilon)$ and an explicit directional
dependence parametrized by the angle $\phi$ with respect to the
$v_{1}$ direction.  With this distribution function the current
density can be evaluated according to
\begin{eqnarray}
    \vec\jmath(x_{2})
    &=&
    2e\int{\rm d}^{2}vf(\vec x,\vec v)\vec v
    \nonumber\\
    &=&
    e\int{\rm d}\epsilon{\cal D}(\epsilon)
    \left(-\frac{\partial f_{0}}{\partial\epsilon}\right)
    \int_{0}^{2\pi}\frac{{\rm d}\phi}{2\pi}
    \chi(x_{2},\phi)\vec v
    \nonumber\\
    &=&
    \frac{e{\cal D}v_{\text F}}{2\pi}\int_{0}^{2\pi}{\rm d}\phi
    \chi(x_{2},\phi)\hat v.
    \label{eqn:j}
\end{eqnarray}
We are using $\vec v\approx\vec v_{\text F}=v_{\text F}\hat v$ and a
constant density of states ${\cal D}(\epsilon)=m/(\pi\hbar^{2})$.

Inserting Eq.~(\ref{eqn:lb}) into the
Boltzmann equation~(\ref{eqn:boltzmann}) gives to linear order
\begin{equation}
    v_{2}\frac{\partial\chi(x_{2},\phi)}{\partial x_{2}}-eEv_{1}=
    \left.
    \frac{\partial\chi(x_{2},\phi)}{\partial t}
    \right|_{\text{scatt}}
    \label{eqn:chi}
\end{equation}
as the determining equation for the unknown $\chi(x_{2},\phi)$.

Following Ref.~\textit{(4)}, we make a relaxation-time
approximation for the bulk impurity scattering part,
\begin{equation}
    \left.\frac{\partial\chi(x_{2},\phi)}{\partial t}\right|_{\text{MR}}
    =
    -\frac{\chi(x_{2},\phi)}{\tau_{\text{MR}}}.
    \label{eqn:chib}
\end{equation}
The momentum-conserving electron-electron scattering part is
parametrized as
\begin{eqnarray}
    \lefteqn{\left.
    \frac{\partial\chi(x_{2},\phi)}{\partial t}
    \right|_{\text{MC}}=}
    \label{eqn:chimc}\\&&
    -\frac{\chi(x_{2},\phi)}{\tau_{\text{MC}}}
    +\frac1{2\pi\tau_{\text{MC}}}
    \int_{0}^{2\pi}{\rm d}\phi'\chi(x_{2},\phi')
    \left(1+2\hat v^{T}\hat v'\right),
    \nonumber
\end{eqnarray}
which is the most simple momentum-conserving form for the scattering
term assuming that the electrons relax to a shifted Fermi-Dirac
distribution $f(\vec x,\vec v)\approx f_{0}(\epsilon-m\vec v^{T}\vec
v_{\text{drift}})$ where the drift velocity is related to the current
density via $\vec\jmath(x_{2})=ne\vec v_{\text{drift}}(x_{2})$, $n:={\cal
D}\mu$ being the electron density.

For the boundary scattering we assume diffusive reflection.  Given a
wire of width $W$, this requires for the solution of
Eq.~(\ref{eqn:lb}) that
\begin{eqnarray}
    \chi(-W/2,\phi)
    &=&
    \frac1\pi\int_{\pi}^{2\pi}{\rm d}\phi'\chi(-W/2,\phi'),
    \\
    \chi(W/2,\phi)
    &=&
    \frac1\pi\int_{0}^{\pi}{\rm d}\phi'\chi(W/2,\phi')
\end{eqnarray}
at the transverse boundaries of the wire.  (We note that
$\phi\in[0,\pi]$ for $x_{2}=-W/2$ and $\phi\in[\pi,2\pi]$ for
$x_{2}=W/2$.)

We introduce an effective mean free path
$\ell_{\text{eff}}(x_{2},\phi)$ describing the average length an
electron at position $x_{2}$ travels in the direction given by the
angle $\phi$ after its last momentum-relaxing scattering event
through the parametrization
\begin{equation}
    \chi(x_{2},\phi)=eE\cos(\phi)\tilde\ell_{\text{eff}}(x_{2},\phi).
    \label{eqn:chiparam}
\end{equation}
From Eqs.~(\ref{eqn:j}) and~(\ref{eqn:chiparam}) it follows that its
angular average
\begin{equation}
    \ell_{\text{eff}}(x_{2})
    :=
    \frac1\pi\int_{0}^{2\pi}{\rm d}\phi
    \cos^{2}(\phi)\tilde\ell_{\text{eff}}(x_{2},\phi)
\end{equation}
is proportional to the drift velocity,
\begin{equation}
    \vec v_{\text{drift}}(x_{2})
    =
    \frac{e\vec E}{mv_{\text F}}\ell_{\text{eff}}(x_{2}).
\end{equation}
Thus defining
\begin{equation}
    {\cal L}_{\text{eff}}:=\frac1W\int_{-W/2}^{W/2}{\rm d}x_{2}
    \ell_{\text{eff}}(x_{2})
\end{equation}
the conductivity of the wire is given by
\begin{equation}
    \sigma=\frac{ne^{2}}{mv_{\text F}}{\cal L}_{\text{eff}}.
\end{equation}

Together with the approximations~(\ref{eqn:chib})
and~(\ref{eqn:chimc}) we insert Eq.~(\ref{eqn:chiparam}) into
Eq.~(\ref{eqn:chi}) and transform the resulting differential
equation into a Fredholm integral equation of the second kind,
\begin{eqnarray}
    \ell_{\text{eff}}(x_{2})
    &=&
    \hat\ell_{\text{eff}}(x_{2})
    \nonumber\\&&{}
    +\lambda
    \int_{-W/2}^{W/2}{\rm d}x_{2}'K(x_{2},x_{2}')
    \ell_{\text{eff}}(x_{2}'),
    \label{eqn:leff}
    \\
    \hat\ell_{\text{eff}}(x_{2})
    :&=&
    \ell-\frac{2\ell}{\pi}\int_{0}^{\pi/2}{\rm d}\phi
    \cos^{2}(\phi)
    \left(
    {\rm e}^{-(W/2+x_{2})/(\ell\sin\phi)}
    \right.\nonumber\\&&\left.{}
    +{\rm e}^{-(W/2-x_{2})/(\ell\sin\phi)}
    \right),
    \\
    K(x_{2},x_{2}')
    &:=&
    \frac1\pi\int_{0}^{\pi/2}{\rm d}\phi\frac{\cos^{2}\phi}{\sin\phi}
    {\rm e}^{-|x_{2}-x_{2}'|/(\ell\sin\phi)}
\end{eqnarray}
with $\lambda:=1/\ell_{\text{MC}}$.  Here we have introduced the
``bare'' mean free path $\ell$ with
$1/\ell:=1/\ell_{\text{MR}}+1/\ell_{\text{MC}}$ and
$\ell_{\text{MC}}:=v_{\text F}\tau_{\text{MC}}$,
$\ell_{\text{MR}}:=v_{\text F}\tau_{\text{MR}}$.

\subsection{Numerics}
\label{sec:numerics}

For given values of the momentum conserving and the momentum relaxing
mean free paths, together with the width of the wire, we eventually
solve Eq.~(\ref{eqn:leff}) numerically: Measuring lengths in units of
$W$ we discretize $x_{2}$ with $N\le100$ segments at
$\{x_{2}=x_{j}:j=1\ldots N\}$ with widths
$\{w_{j}:j=1\ldots N\}$ between the $\pm W/2$ boundaries and replace
the integration over the kernel $K$ in each of the $N$ partitions by a
mean value, mapping the solution onto a matrix problem, written in
components
\begin{equation}
    \ell_{i}-\lambda\sum_{j=1}^{N}K_{ij}w_{j}\ell_{j}
    =
    \hat\ell_{i},
    \quad
    i=1\ldots N
    \label{eqn:matrix}
\end{equation}
with $K_{ij}:=K(x_{i},x_{j})$ and equivalently for $\ell$ and
$\hat\ell$.  The solutions to this linear system can be found easily
as long as $\lambda\equiv(\ell_{\text{MC}}/W)^{-1}$ is not too large,
i.\,e.  for weak electron-electron scattering.  In the opposite case
$\ell_{\text{MC}}/W\ll1$, Eqs.~(\ref{eqn:leff}) and~(\ref{eqn:matrix})
become numerically unstable.  To overcome this instability, we solve
the equivalent problem
\begin{eqnarray}
    \lefteqn{\ell_{\text{eff}}(x_{2})\left(
    1-\lambda\int_{-W/2}^{W/2}{\rm d}x_{2}'
    K(x_{2},x_{2}')\right)=}
    \\
    &&
    \hat\ell_{\text{eff}}(x_{2})
    +
    \lambda
    \int_{-W/2}^{W/2}{\rm d}x_{2}'K(x_{2},x_{2}')
    \left(
    \ell_{\text{eff}}(x_{2}')
    -\ell_{\text{eff}}(x_{2})
    \right),
    \nonumber
\end{eqnarray}
again mapping it onto a matrix problem as before.
Fig.~S5 displays the resulting dependence of the
resistivity $\rho$ on the ratio $\ell_{\text{MR}}/W$ for fixed values
$\ell_{\text{MC}}/\ell_{\text{MR}}$.

\subsection{Viscous flow of charged particles}

In this section, we present a calculation of the flow of charged
particles through a two-dimensional channel in the fully hydrodynamic
limit, i.\,e. when momentum is fully conserved in the bulk of the fluid.
We start from Newton's second law $\rho\dot{\vec v}=\vec g$,
introducing a mass density $\rho:=m\int{\rm d}^{2}vf(\vec x,\vec v)$
and a force field $\vec g(\vec x)$.  The electrons are subject to two
forces, (a) shear forces characterized by a finite viscosity, and (b)
an electrostatic field gradient along the wire in direction $x_{1}$
(Lorentz force).  We regard the electrons as an incompressible fluid
and ignore all momentum relaxing processes.  In particular we assume
that no point scatterers are present in the wire.

The shear modulus of an infinitesimally small cube inside the fluid is
\begin{equation}
    S_{ij}:=\eta\left(\frac{\partial v_{i}}{\partial x_{j}}+
    \frac{\partial v_{j}}{\partial x_{i}}\right),
\end{equation}
and the $i$th component of the corresponding force field thus is
\begin{eqnarray}
    g_{i}
    &=&
    \sum_{j}\frac{\partial S_{ij}}{\partial x_{j}}
    =
    \eta\left[
    \left(\sum_{j}\frac{\partial^{2}}{\partial x_{j}}\right)v_{i}
    +\frac{\partial}{\partial x_{i}}
    \left(\sum_{j}\frac{\partial v_{j}}{\partial x_{j}}\right)
    \right],
    \nonumber
\end{eqnarray}
where the second term inside the square brackets vanishes due to the
incompressibility of the electrons ($\nabla\vec v\equiv0$).  Together
with the electric field $\vec E$ along the wire we have to solve the
equation
\begin{equation}
    \rho\dot{\vec v}=\eta\Delta\vec v-\rho\frac em\vec E,
\end{equation}
which is equivalent to the Navier-Stokes equation for a stationary
laminar flow of an incompressible fluid.  We seek a steady state, so
$\dot{\vec v}=0$ as well.  With $\vec E=-(V/L)\hat x_{1}$ for our wire
with length $L$ and width $W$ ($\hat x_{i}:=x_{i}/|\vec x|$), the
solution is given by $\vec v=v(x_{2})\hat x_{1}$,
\begin{equation}
    v(x_{2})=\frac12\frac\rho\eta\frac emE
    \left(x_{2}^{2}-\frac{W^{2}}{4}\right)
\end{equation}
for $-W/2\le x_{2}\le W/2$.  With
$n=\rho/m$, this causes a current
\begin{equation}
    I
    =
    neT\int_{-W/2}^{W/2}{\rm d}x_{2}v(x_{2})
\end{equation}
through the wire of thickness $T$ (being infinitely smooth at
$x_{3}=\pm T/2$), and we obtain for the resistance $R=V/I$
\begin{equation}
    R=\frac{12 L}T\frac{\eta}{(ne)^{2}}
    \frac1{W^{3}}.
    \label{eqn:r}
\end{equation}
We note that the finiteness of the resistance is exclusively due to
the finite width of the wire: Because the electronic momentum is
conserved, we must have $R\to0$ in the bulk limit.

\subsection{Intuitive significance of the de Jong-Molenkamp theory}

The comparison of Eq.~(\ref{eqn:r}) with the solid line in
Fig.~S5 is significant.  Resistance $R$ varying as $1/W^3$
is equivalent to resistivity $\rho$ varying as $1/W^2$ because of the
extra geometrical factor $TW/L$ in the definition of $\rho$.  The
quadratic extra contribution to $\rho$ in the calculation of
sections~\ref{sec:dejong} and~\ref{sec:numerics} at high rates of
momentum-conserving scattering
($\ell_{\text{MC}}/\ell_{\text{MR}}\to0$) is therefore naturally
identified with a viscous contribution to the resistivity.  In the
opposite limit when the rate of momentum-conserving scattering tends
to zero ($\ell_{\text{MC}}/\ell_{\text{MR}}\to\infty$) the dotted line
limits to the ballistic transport result calculated in theories that
ignore momentum-conserving scattering~\textit{(30)}. Since the
theory limits to physically reasonable results at both its extremes,
we believe that some confidence can be placed in its predictions.
When plotted in the dimensionless units of Fig.~S5, these
predictions are unique for each value of
$\ell_{\text{MC}}/\ell_{\text{MR}}$, and contain no free parameters.
In other words, both the functional form and the magnitude of the
change in resistivity as a function of channel have physical
significance.  In this context, the closeness of the prediction for to
the experimental data shown in Fig.~4A of the main paper for
$\ell_{\text{MC}}/\ell_{\text{MR}}=0.1$ is very good.

The $1/W^3$ variation predicted for $R$ at
$\ell_{\text{MC}}/\ell_{\text{MR}}=0.005$ gives the opportunity to
calibrate $\rho/\rho_0-1$ against viscosity.  Specifically, for
$\ell_{\text{MC}}/\ell_{\text{MR}}\ll1$, we approximately have
\begin{equation}
    \frac{\rho}{\rho_{0}}
    \approx
    1+b\left(\frac{\ell_{\text{MR}}}{W}\right)^{2},
    \label{eqn:rapprox}
\end{equation}
with a coefficient $b$ strongly depending on the exact
$\ell_{\text{MC}}/\ell_{\text{MR}}$ ratio.  We note that in the strong
electron-electron scattering limit we are at the border of validity of
the theory, mirrored by the fact that we suffer from numerical
instabilities when solving Eq.~(\ref{eqn:leff}) for
$\ell_{\text{MC}}/\ell_{\text{MR}}\lesssim0.005$.  With these
ambiguities in mind, we obtain an estimate $b={\cal
O}(10^{-3}\ldots10^{-2})$.

\section{Analysis of experimental data using hydrodynamic theory}

\subsection{Estimate of viscosity}
For analyzing the actual experimental data from PdCoO$_{\text2}$, we
first note that the momentum conserving scattering processes relevant
to our experiment likely include normal electron-phonon events (since
the strong phonon drag prevents these from relaxing the momentum of
the electron assembly) as well as electron-electron events.  However,
both types of processes can safely be encoded by the parameter
$\ell_{\text{MC}}$ for the purposes of our analysis, since it is
performed at fixed temperature.  A more sophisticated theory would be
required to extend it reliably to situations in which the temperature
is varied.

Next, we estimate the viscosity $\eta$.  First we note that
comparison of Eqs.~(\ref{eqn:r}) and~(\ref{eqn:rapprox}) implies that
\begin{equation}
    b
    =
    \frac{12\eta}{(ne)^{2}\rho_{0}\ell_{\text{mr}}^{2}}.
\end{equation}
Taking the estimate of the value of $b$ obtained from here, using the
known values for $n$, $e$, $\ell_{\text{MR}}$ and $\rho_{0}$
($4.9\times10^{28}\,\rm m^{-3}$, $1.602\times10^{-19}\,\rm C$,
$2\times10^{-5}\,\rm m$ and $8\times10^{-11}\,\Omega\rm m$
respectively) and working at our maximum measured value of
$\ell_{\text{MR}}/W=20$, for which $\rho/\rho_{0}-1\approx4$ for
$\ell_{\text{MC}}/\ell_{\text{MR}}=0.005$ (Fig.~S5, solid
line), we obtain $\eta$ in the range
$1.6\times10^{-4}\ldots1.6\times10^{-3}\,{\rm kg}({\rm m\,s})^{-1}$.
Converting this unambiguously to the viscous contribution to our
experimental data at $\ell_{\text{MR}}/W=20$ would require being able
to decouple the viscous effects on boundary scattering from those
associated with the impurity scattering.  This is possible for the
$\ell_{\text{MC}}/\ell_{\text{MR}}\to\infty$ limit (impurity
scattering dominates) and $\ell_{\text{MC}}/\ell_{\text{MR}}\to0$
(viscous effects dominate) but cannot be done with certainty for the
parameter range ($\ell_{\text{MC}}/\ell_{\text{MR}}\approx0.1$)
relevant to the experiments.  However, two limits can be established
on the viscous contribution to the experimental data.  One extreme is
to attribute the entire extra resistivity to viscous effects, i.e. to
set $(\rho/\rho_0-1)_{\text{visc}}=14$.  The other is to attribute the
viscous contribution only to the difference between the measured data
and the boundary scattering that would have resulted in the absence of
any momentum conserving scattering processes.  This sets
$(\rho/\rho_0-1)_{\text{visc}}=6$.  The true viscous contribution must
lie between these limits, yielding an estimate for the viscosity of
the electron fluid in PdCoO$_{\text{2}}$ of $\eta$ between
$3\times10^{-4}$ and $6\times10^{-3}\,{\rm kg}({\rm m\,s})^{-1}$.

Viscosities of everyday fluids are typically quoted either as dynamic viscosity $\eta$ as given above, or as kinematic viscosity $\nu$, obtained by dividing out the mass density.  Doing that for our PdCoO$_{\text{2}}$ results gives 0.01~m$^2$s$^{-1}$$<\nu<$ 0.3~m$^2$s$^{-1}$.  In a Fermi liquid, $\nu$  can be estimated as $\alpha\nu{_F}\ell_{MC}$ , with $\alpha \sim$0.2 \textit{(38)} .  Fig.~4 of the main paper show that our data are consistent with $\ell_{MC}$$\sim$2~$\mu$m, and $\nu{_F} $ for PdCoO$_{\text{2}}$ is approximately 7.5 $\times$ 10$^5$ ms$^{-1}$ ~\textit{(18)} , giving a second estimate for $\nu$ that falls within our quoted range.  This is a useful internal cross-check on our method for estimating viscosity.  Taken together, these analyses mean that the electron fluid in PdCoO$_{\text{2}}$ has a dynamic viscosity similar to that of water (1$\times$10$^3$~kg(ms)$^{-1}$ at room temperature) but a kinematic viscosity greater closer that of honey ($\sim$0.01~m$^2$s$^{-1}$  at room temperature).

After submission of our manuscript, a report of measurements of the viscosity of the electron fluid in graphene appeared on the archive~\textit{(39)}.  For those samples the kinematic viscosity is similar to that deduced here for PdCoO$_{\text{2}}$, but the dynamic viscosity is approximately 10$^4$ smaller due to the low carrier concentration.

\subsection{Effect of varying $\ell_{MC}/\ell_{MR}$  by changing sample temperature}
As discussed in the main text, the theory of Ref.~\textit{(4)} cannot be expected to directly calculate temperature dependent hydrodynamic effects in PdCoO$_2$ accurately because it is likely to have different temperature dependent sources for its momentum-conserving scattering than those expected in the low carrier density two-dimensional electron gas for which the theory was designed.  However, one can anticipate that, by changing the temperature, one can alter the $\ell_{MC}/\ell_{MR}$ ratio.  Since the Fermi temperature of PdCoO$_2$ is so high (approximately 30000 K) that all thermally-induced momentum-relaxing scattering at room temperature and below is quasi-elastic, this is similar to studying the effects of changing residual resistivity, but with an unknown accompanying change to $\ell_{MC}$.  Although the $\ell_{MC}$ change is not controlled, such an experiment has the capability of checking for sensitivity to momentum-conserving scattering, as outlined in Figs.~S6 A and B.  In each figure, the $\ell_{MC}/\ell_{MR}$ ratio is changed by a factor of 20 by starting from different assumed values of $\ell_{MC}/\ell_{MR}$ and varying $\ell_{MR}$ .  In Fig. S6 A, where the starting value is 0.05 is in the region deduced from the analysis accompanying Fig.~4 C of the main paper, changing the ratio by decreasing $\ell_{MR}$ results in predicted changes to the data because the viscous contribution to the boundary scattering is being changed.  In Fig.~S6 B, in contrast, the only change resolved is restriction of the accessible $\ell_{MR}/W$ range.  This is because in this range of $\ell_{MC}/\ell_{MR}$ the momentum-conserving scattering is too weak to affect the resistance, and all the curves are essentially the same as the standard transport theory curve of Fig.~4 in the main paper.

 In Fig.~S6 C we present analysis of data at 20, 30, 40, 50, and 75~K, a range across which  $\ell_{MR}$ changes substantially, by amounts that can be deduced from the restriction along the $\ell_{MR}/W$ axis.  The curves ``fan out'' from each other like the data predicted in Fig.~S6~A, rather than following the near-universal curve predicted in Fig.~S6~B or the completely universal curve that would be predicted by traditional transport theory.  We believe that this is further evidence that momentum-conserving scattering and hence electronic hydrodynamics play an important role in determining the resistance of our channels.

\pagebreak

\begin{figure}[t]
	\begin{center}
	\includegraphics[width=11 cm]{FigS1.eps}
	\end{center}
	\caption{\baselineskip1.5em\label{S1} The sample fabricated to check current flow and electrical thickness as a function of length along our device.  The voltage contacts are spaced with a separation approximately a factor of three closer together than on the device shown in Fig.~1 of the manuscript, allowing determination of the electrical thickness of that sample as described in the text. Current is injected through the top contacts marked `I'.}
\end{figure}

\begin{figure}[t]
	\begin{center}
	\includegraphics[width=8 cm]{FigS2.eps}
	\end{center}
	\caption{\baselineskip1.5em\label{S2} Width and height determination in the SEM for a sample around $W$~=4~$\mu$m. In this case, $W_{top}$~=3.2~$\mu$m and $W_{bottom}$~=4.5~$\mu$m, yielding a weighted average width of $W$=4.06~$\mu$m.}
\end{figure}

\begin{figure}[t]
	\begin{center}
	\includegraphics[width=10 cm]{FigS3.eps}
	\end{center}
	\caption{\baselineskip1.5em\label{S3} Ga implantation and damage range in PdCoO$_2$ for high angle incidence (87.5$^o$).}
\end{figure}

\begin{figure}[t]
	\begin{center}
	\includegraphics[width=14 cm]{FigS4.eps}
	\end{center}
	\caption{\baselineskip1.5em\label{S4} PdCoO$_{2}$ microstructure designed for consistency checks of the resistivity scaling with conductor length. The main current path is highlighted in purple. The current is injected into the structure through large meandered paths, to ensure current homogeneity in the central bar.}
\end{figure}

\begin{figure}
    \centering
    \includegraphics[width=\columnwidth]{FigS5.pdf}
    \caption{\baselineskip1.5em\label{S5} Dependence of the resistivity $\rho$ normalized to the
    bulk resistivity $\rho_{0}$ on the ratio $\ell_{\text{MR}}/W$ at
    fixed $\ell_{\text{MC}}/\ell_{\text{MR}}=0.005$ (solid line,
    strong electron-electron scattering), $0.1$ (dashed line), and
    $1000$ (dotted line, weak electron-electron scattering).}
    \label{fig:rho}
\end{figure}

\begin{figure}[t]
	\begin{center}
	\includegraphics[width=9.5 cm]{FigS6.eps}
	\end{center}
	\caption{ \baselineskip1.5em \label{S6} A and B:  Predictions of the hydrodynamic theory over similar dynamic ranges of $\ell_{MC}/\ell_{MR}$  but different starting values.  In A they are seen to fan out because in that part of the predicted phase diagram the results have sensitivity to changes in $\ell_{MC}/\ell_{MR}$ , while in B they follow a quasi-universal curve.  In C we show data from PdCoO$_2$ in which the $\ell_{MC}/\ell_{MR}$  ratio is tuned by raising the temperature. Lines are guides to the eye made using second-order polynomials, not fits to the theory. The precise changes to $\ell_{MC}/\ell_{MR}$ are not known, so the test is only qualitative, but the data are seen to be consistent with the prediction in panel A and definitely not consistent with the prediction in panel B.}
\end{figure}
\end{document}

redpajama_set_name: RedPajamaArXiv


Microsoft plans to start a small-scale pilot of a microblogging service aimed at business users that it has been experimenting with in Office Labs.
It didn't reveal many details of the service but said it has been testing it internally and the company is now looking for customers willing to participate in a pilot test.
Called OfficeTalk, the service is designed to let employees share brief bits of information, similar to the way that people use Twitter. "This concept test applies the base capabilities of microblogging to a business environment, enabling employees to post their thoughts, activities, and potentially valuable information to anyone who might be interested," according to a blog post on the Office Labs site.
OfficeTalk was one of the most popular internal concept tests at Office Labs, the post says.
"Not only was the obvious demonstrated, that people don't limit microblogging activity to the purely social, but that even an IT managed implementation focused on business productivity can spread quickly across informal networks and create unique collaboration efficiencies and experiences," it said.
Microsoft now wants to test OfficeTalk along with other social-networking experiments with a few customers. It hopes to study ways that businesses and people use the technologies, according to the blog post.
Microsoft is following other companies that are already offering microblogging software for enterprises. For instance, SocialText, StatusNet, Yammer, Socialcast and Salesforce's Chatter are all microblogging products used by enterprises.
Office Labs researchers are always quick to point out that they work on experiments that may never become live products, and this blog post is no different. "OfficeTalk isn't a product -- it's a research project focused on learning how people might use social networking tools at work and in what ways both people and organizations realize their value," it reads.
The blog post is dated Wednesday, and ZDNet wrote about it on Friday.


text:
Q: Display of a large amount of data in a Canvas with a Scrollbar I'm having a problem trying to display a large table in tkinter.
First, I tried to display all label at once in the canvas, but over few hundred rows, the program shut down. So I tried to create a scrollable canvas that updates everytime I scroll: I collect the position of the scrollbar and depending on the position of it, I display the 10 values corresponding.
But I can't get this code working. For now it only displays a black background with the scrollbar on the right.
Here is the code:
from tkinter import *

class Application(object):
    def __init__(self, parent):
        self.x = []
        for i in range(1, 1000):
            self.x.append(i)
        self.parent = parent
        self.mainFrame =  Frame(self.parent)
        self.mainFrame.pack()
        self.canvas = Canvas(self.mainFrame, width = 200, height = 500, bg = "black")
        self.canvas.grid(row = 0, column = 0)
        self.scroll = Scrollbar(self.mainFrame, orient = VERTICAL, command = self.update)
        self.scroll.grid(row = 0, column = 1)

        self.canvas.configure(yscrollcommand = self.scroll.set)
        self.tabCursor = 0
        self.scrollPosition = self.scroll.get()

    def update(self):
        self.tabCursor = round(self.scrollPosition[0]*len(self.x))
        if ((len(self.x) - self.tabCursor) < 10):
            self.tabCursor = len(self.x) - 10
        for i in range(0, 10): #display 10 values
            label = Label(self.canvas, text = str(self.x[tabCursor + i]), width = 50)
            label.grid(column = 0, row = i)

if __name__ == '__main__':
    root = Tk()
    app = Application(root)
    root.mainloop()

EDIT :
I finally had time to implement your answer. It looks fine but I can't get the scrollbar working and i don't know why.
class TableauDeDonnees(object):
    "Tableau de données -- Onglet Tableau de données"
    def __init__(self, data, parent):
        self.parent = parent
        self.data = data
        print(self.data[0], self.data[1])
        print(len(self.data[0]), len(self.data[1]))
        self.labels = []
        self.navigationFrame = Frame(self.parent)
        self.canvas = Canvas(self.parent, bg = "black", width = 200, height = 500)
        self.mainFrame = Frame(self.canvas)
        self.navigationFrame.pack()
        print(len(data))
        for row in range(50):
            for column in range(len(data)):
                self.labels.append(Label(self.canvas, text = str(data[column][row])))
        for i in range(len(self.labels)):
            self.labels[i].grid(row = i // 2, column = i % 2, sticky = NSEW)
        self.boutonRetour = Button(self.navigationFrame, text = "Retour", command = lambda: self.move(-2))
        self.quickNav = Entry(self.navigationFrame, width = 3)
        self.quickNav.bind('<Return>', lambda x: self.move(self.quickNav.get()))
        self.boutonSuivant = Button(self.navigationFrame, text = "Suivant", command = lambda: self.move(0))

        temp  = divmod(len(data[0]), len(self.labels) // 2)
        self.pages = temp[0] + (1 if temp[1] else 0)

        self.position = Label(self.navigationFrame, text='Page 1 sur ' + str(self.pages))
        self.pageCourante = 1

        self.boutonRetour.grid(row = 0, column = 0)
        self.quickNav.grid(row = 0, column = 1)
        self.boutonSuivant.grid(row = 0, column = 2)
        self.position.grid(row = 0, column = 3)

        self.scroll = Scrollbar(self.parent, orient = VERTICAL, command = self.canvas.yview)
        self.canvas.configure(yscrollcommand = self.scroll.set)
        self.scroll.pack(side = RIGHT, fill='y')
        self.canvas.pack(side = LEFT, fill = 'both')

        self.canvas.create_window((4,4), window = self.mainFrame, anchor = "nw", tags = "frame")
        self.canvas.configure(yscrollcommand = self.scroll.set)
        self.mainFrame.bind("<Configure>", self.update)
        self.canvas.configure(scrollregion = self.canvas.bbox("all"))

    def update(self, event):
        self.canvas.configure(scrollregion = self.canvas.bbox("all"))

    def move(self, direction):
        if (self.pageCourante == 1 and direction == -2) or (self.pageCourante == self.pages and direction == 0):
            return
        if direction in (-2, 0):
            self.pageCourante += direction + 1
        else:
            try:
                temp = int(direction)
                if temp not in range(1, self.pages + 1):
                    return
            except ValueError:
                return
            else:
                self.pageCourante = temp
        for i in range(len(self.labels)):
            try:
                location = str(self.data[i % 2][len(self.labels)*(self.pageCourante - 1) + i])
            except IndexError:
                location = ''
            self.labels[i].config(text = location)
        self.position.config(text = 'Page ' + str(self.pageCourante) + ' sur ' + str(self.pages))

I don't understand why the scrollbar isn't working properly. Note, that my parent is a notebook.
Also, there is a problem with the number of items displayed. The number of pages is right but it seems it displays more than it should cause last pages are empty and the last values displayed seems right.
Thank you for your attention

A: The scrollbar doesn't work by continuously creating new widgets ad infinitum. You were also missing some key parts - unfortunately, Scrollbar isn't as straightforward as most tkinter widgets.
from tkinter import *

class Application(object):
    def __init__(self, parent):
        self.parent = parent
        self.canvas =  Canvas(self.parent, bg='black', width = 200, height = 500)
        self.mainFrame = Frame(self.canvas)
        self.scroll = Scrollbar(self.parent, orient = VERTICAL, command=self.canvas.yview)
        self.canvas.configure(yscrollcommand=self.scroll.set)
        self.scroll.pack(side='right', fill='y')
        self.canvas.pack(side='left', fill='both')
        self.canvas.create_window((4,4), window=self.mainFrame, anchor="nw", tags="frame")

        self.canvas.configure(yscrollcommand = self.scroll.set)
        self.mainFrame.bind("<Configure>", self.update)
        self.x = []
        for i in range(1000):
            self.x.append(Label(self.mainFrame, text=str(i)))
            self.x[i].grid()

    def update(self, event):
        self.canvas.configure(scrollregion=self.canvas.bbox("all"))

if __name__ == '__main__':
    root = Tk()
    app = Application(root)
    root.mainloop()

If you'd like to show only a few at a time and provide a forum-like interface, you can use Buttons to navigate between pages. This example allows the user to navigate with Back and Forward buttons, as well as by entering a page number in the box and pressing Enter.
from tkinter import *

class Application(object):
    def __init__(self, parent):
        self.x = list(range(1000))
        self.labels = []
        self.parent = parent
        self.navigation_frame = Frame(self.parent)
        self.canvas =  Canvas(self.parent, bg='black', width = 200, height = 500)
        self.mainFrame = Frame(self.canvas)
        self.navigation_frame.pack()
        for i in range(100):
            self.labels.append(Label(self.mainFrame, text=str(i)))
            self.labels[i].grid()
        self.back_button = Button(self.navigation_frame, text='Back', command=lambda: self.move(-2))
        self.quick_nav = Entry(self.navigation_frame, width=3)
        self.quick_nav.bind('<Return>', lambda x: self.move(self.quick_nav.get()))
        self.forward_button = Button(self.navigation_frame, text='Forward', command=lambda: self.move(0))

        temp = divmod(len(self.x), len(self.labels))
        self.pages = temp[0] + (1 if temp[1] else 0)

        self.you_are_here = Label(self.navigation_frame, text='Page 1 of ' + str(self.pages))
        self.current_page = 1
        self.back_button.grid(row=0, column=0)
        self.quick_nav.grid(row=0, column=1)
        self.forward_button.grid(row=0, column=2)
        self.you_are_here.grid(row=0, column=3)
        self.scroll = Scrollbar(self.parent, orient = VERTICAL, command=self.canvas.yview)
        self.canvas.configure(yscrollcommand=self.scroll.set)
        self.scroll.pack(side='right', fill='y')
        self.canvas.pack(side='left', fill='both')
        self.canvas.create_window((4,4), window=self.mainFrame, anchor="nw", tags="frame")

        self.canvas.configure(yscrollcommand = self.scroll.set)
        self.mainFrame.bind("<Configure>", self.update)

    def update(self, event):
        self.canvas.configure(scrollregion=self.canvas.bbox("all"))

    def move(self, direction):
        if (self.current_page == 1 and direction == -2) or (self.current_page == self.pages and direction == 0):
            return
        if direction in (-2, 0):
            self.current_page += direction + 1
        else:
            try:
                temp = int(direction)
                if temp not in range(1, self.pages+1):
                    return
            except ValueError:
                return
            else:
                self.current_page = temp
        for i in range(len(self.labels)):
            try:
                location = str(self.x[len(self.labels)*(self.current_page - 1) + i])
            except IndexError:
                location = ''
            self.labels[i].config(text=location)
        self.you_are_here.config(text='Page ' + str(self.current_page) + ' of ' + str(self.pages))

if __name__ == '__main__':
    root = Tk()
    app = Application(root)
    root.mainloop()


text:
require 'observer'

module DRb
  module DRbObservable
    include Observable

    def notify_observers(*arg)
      if defined? @observer_state and @observer_state
        if defined? @observer_peers
          @observer_peers.each do |observer, method|
            begin
              observer.send(method, *arg)
            rescue
              delete_observer(observer)
            end
          end
        end
        @observer_state = false
      end
    end
  end
end

redpajama_set_name: RedPajamaGithub


downstairs that the previous owners have set up as an office with built-in shelving. One full bath downstairs. Upstairs there are 3 bedrooms including the master bedroom. Master bath has double vanity with standup shower and large closet. Two of the upstairs bedrooms have walk-in closets. There are hurricane shutters across the front of this magnificent home. Two parking pads at the front with brick walkways up to the front door and leading around to the back. There is a Play Park & small Lake in Forest Hills neighborhood along with Tennis Courts. No HOA. Call today to schedule a viewing of this executive home.


At IDS + Co we can advise businesses in the Scotland area on the possible tax advantages of employing your spouse in the firm. Here is an overview of the issues.
If you are in the Scotland area and are considering employing your spouse in your business, IDS + Co can advise you of the tax advantages and other implications.


Cape Cobras will take on Warriors for the First match of Momentum One Day Cup 2019, is going to be played on 8 February, Friday at Boland Park, Paarl. CC Vs WAR 1st ODI South Africa ODD 2019 Dream11 prediction is given in this post with all key stats.
JP Duminy is unavailable for the opening match.
Dane Piedt will lead the team in Duminy's absence.
Dayyaan Galiem and Mthiwekhaya Nabe ruled out from this match.
Isaac Dikgale and Akhona Mnyaka replace them in the squad.
Colin Ackerman in not available for the first match.
Marco Marais and Gihahn Cloete will open the batting for team.


Where can I find information and data on remittances?
Start with the Migration and Remittances page from World Bank, and their Factbook. It provides detailed data including bilateral flows for many nations.
UNCTADSTAT also includes remittances back to 1980.
The Migration Policy Institute offers statistics, reports, factbooks, maps and more information about migration.
For information on remittances in the Western Hemisphere, go to the Inter-American Development Bank Remittances Site.
For background information on remittances from Spain, see the INE. Access Inebase via E-Resources List.
To find books on this topic, search under the subject "emigrant remittances" in the IESE Library catalog.


This beautiful bi-level single family home has been completely renovated. With a brand new kitchen with granite counter tops, new cabinets, stove & dishwasher. New sliding glass doors opens up to a raised deck. Updated Bathrooms! New carpets in bedrooms, beautiful hardwood floors in dining room & living room. Wood burning stove in family room.
This amazing one-of-a-kind home ties together the traditional, historic design with a touch of modern flair to give this property a touch of elegance & sophistication. Located on almost 4 acres on River Road you have to see the property to get a true appreciate of all it has to offer.


SEI/Aaron''s is Aaron''s largest franchisee operating over 100 stores in 10 states.
Our Company is growing fast! In the last two years we have added 20 stores with a goal of being over 200 stores by 2018. At SEI/Aaron's we carry a huge selection of brand name furniture, electronics, computers and appliances. Our sales associates have to deal with minimal paperwork and have the benefit of high volume walk-in traffic.
You will help customers that call or come into the store find the merchandise they want and need. Best of all, you don''t have to worry about qualifying the customer for the merchandise they want. Just sell, sell, sell!


YouTube: I watch a lot of videos about productivity, planning, planner set-ups, etc. As such, it's hardly surprising that I eventually stumbled across videos about digital planning. I use a Happy Planner, so I'm already used to being able to customize my planner because it's a discbound system that allows pages to be moved around and added. Seeing how much more customization was possible with a digital planner really appealed to me, as my handwriting is terrible and I have no need for so much crafting supplies. I use creative projects to help de-stress during tough points in the semester, so about mid-April I started looking for how-to videos about creating digital planners. I definitely credit the videos by LLovesMac89 as the ones that allowed me to create my own planner pretty quickly and easily.
Keynote: This is the Apple app that I used to create the hyperlinked PDFs. By hyperlinked, I mean that every planner tab on every page is a link so that you can maneuver through the PDF quickly. Want to open up your planner and go straight to your second project? Just click on the second project tab on whatever page you're on and you'll go directly to that project's first page in the PDF. Figuring out how to mask shapes was a slight struggle, but once I figured it out, it was so much fun to create the "planner" and its tabs. I'll talk more about masking shapes in next week's post about digital "stickers." I also made a few digital notebooks with this app, so that I could try out bullet journaling or note-taking via my iPad.
Good Notes: To actually use the digital academic planner I created, I bought this app for $7.99. It's incredibly user-friendly, in my opinion, and it makes reading and annotating PDFs so easy. It takes a few tries to understand the various settings, but once you get into the rhythm, you'll start finding additional reasons to use this app, if you don't already. While the planner should work with some other PDF annotators, this is the only app I've used so it's the one I focus on in my tutorial below. In case you want to consider other productivity tools alongside your planner, here are a few other digital tools to try out.
MagicEraser: This is a free app that allows you to erase certain parts of images. So, you can design headings, graphs, stickers, etc. and then "erase" the white space behind and around these things so that they are all that's left to paste into the planner pages. So, for example, if you create a header for each month in Word, you can take a screenshot of that page, then "erase" the background so that all that's left are the words. There are a lot of free "stickers" and icons to be found online (Pinterest), so using this app can help liven up your planner, if you're interested.
There are quite a few hyperlinked tabs in the planner. They start with the academic year (July-June), followed by four tabs for projects that you're working on. The tab at the top of the left page will take you to the fourth page of the PDF, in case you want to add some pages before July begins on the fifth page (i.e. year at a glance pages, contact lists, deadlines list, "sticker" pages, etc.). The three tabs at the top of the right page have no labels, so you can make those sections into whatever you want. Each of those three tabs are linked to the very "back" of the planner, after the project pages.
Side Note: The second and third pages in the PDF are not intended to be written/typed on. They are the blank templates you can use when customizing your planner (more on that later).
The blank pages can be used for making lists (goals, tasks, events) or anything else you find relevant to add to that month. I start each week on Monday, so the final rectangle on the second page is split into Saturday and Sunday. If you don't like how the rectangles look, you can delete them and just add more of the blank pages so that you have enough for each month (more on that below). For example, you can add a page for each day and make it a daily planner, rather than a weekly planner.
These pages come in the planner, though you can add as many as you need for each project. You can import images into Good Notes really easily, so you could always screenshot or scan documents and then paste them into these sections. You can also use these sections for brainstorming, outlining, tracking progress, writing to-do lists, etc.
The three tabs on the top right of the planner spread link to sections that each have 10 pages, but you can add more or less pages as needed. You can use these tabs for whatever you want, or never use them. A few potential uses: self-care ideas and habit tracking, icons/stickers for planner use, meal planning, contact lists, master lists of deadlines, etc. If you're a teacher, you might want to use one of these sections as a teaching journal. Or, you can use a section to brainstorm your routines, habits, goals, projects, etc. Here's a post about making the best of a new year.
If you don't want to experiment with adding, subtracting, or moving around various pages, you could still consider how you want to approach filling out the planner. Do you have a stylus you can use to write with or are you going to use the text box function? Both? Are you going to color code? Do you want to add images and icons or just text? To give you some ideas, here are a couple screenshots with examples of how you can use the weekly pages in the calendar part of your planner. I created the icons that appear in the second image using Keynotes. I'll discuss the process of making these icons/stickers in my next post.
What if you want to design your own weekly layouts or want to make this a daily planner because you have so much going on every day of the week? With Good Notes, changing this PDF into one you can customize in this way is easy, as it only takes a few simple steps, repeated as many times as needed.
Step 1: Click the four-box icon at the top left of the screen (once your planner PDF is open), then click Edit.
Step 2: In the thumbnails, click on a blank page with no boxes. An orange border will appear around its edges once you've selected it.
Step 3: Clip Copy, then Done.
Step 5: Keep adding pages as many times as you want/need. You can always add more later following these same steps. Once you've added what you want, click Done.
Hint: If you want to still use the design of a full week on one page spread, but don't like the rectangle look, just paste 6 blank pages to each month (click on each month tab and it will take you to the first page of that month). But, let's say you want to add 16 blank pages after the first page spread of July (so that you can have one full page devoted to each day for the whole month). If you want this daily planner setup for all the following months, you can start with step 1 above, click on all 16 pages you've just added, copy them, then paste them after the first page spread of each month. You'll now have a daily planner rather than the weekly one that I created. Of course, copying 16 pages means that extra page(s) will be included for each month, since no month has 32 days. You can always delete the extra for each month, if that bothers you. Here's an example of how you can use this latter design.
Step 6: To get rid of the weekly pages with boxes, just follow steps 1 and 2, select all the pages with weekly boxes, and then click Delete.
Voila! You have now converted the monthly planner portion into a completely customizable system, whether that means just a weekly planner filled with blank pages or a daily planner. You now know how to add more pages to the other sections, as well.
Side note: Very similar steps can be used to move around pages in your planner, so you can keep certain types of notes or documents together without having to worry about completing them all at once or leaving empty page spreads in anticipation of more notes/documents about a certain topic/project stage being added later. For example, if you brainstormed for a project and then started to outline it, but then decide the next day to brainstorm more before continuing the outline, you can just add a new blank page between the brainstorming and outlining that you've already done.
Now that I've gone over the basics, here are the links to the two PDFs I've made. I can't guarantee that there are no mistakes with the hyperlinks, as this creative project is still pretty new to me. I've tried them both out, though, and haven't encountered any issues with these versions. Both digital academic planners – this colorful one and this grayscale one – have the same structure, so I'll just add an image of the colorful one below since this version didn't appear in the above tutorial. Also, while they each have 158 pages, the colorful one is a slightly larger file (7.7 MB vs 7 MB, after being compressed). If you'd rather use a blank digital notebook to plan, here's the post with those PDFs.
In my next post, I'll focus more on helpful resources for learning more about digital planning, and I'll also go over the process of making digital "stickers." There are more professionally made digital planners out there, so I'll link to a few of them in the next post for anyone who might decide that digital planning is definitely for them and they want an upgrade before really diving in next month (I promise, my feelings won't be hurt). Of course, YouTube or Pinterest are the best resources if you want to get a head start on further customizing your planner before my next post.
Do you use a digital planner or plan to start now? If so, I'd love to hear about your favorite, obscure elements of this type of planning.
The BEST Assessment Tool to Use Midway through the Semester?


text:
The Greats: Learning Strategies of Master Forensic Psychiatrists
Graham Glancy University of Toronto
Daniel Miller University of Toronto
https://doi.org/10.15173/ijrr.v4i1.3911
Forensic psychiatry, deliverate practice model, career management, professional development
For forensic psychiatry to thrive as a profession, practitioners need to be committed to intentional, continuous learning and development throughout their careers. However, carving their way through the challenges of practice and finding room to grow can be daunting. Research can help lessen this burden by examining the careers of experienced and skilled practitioners, identifying the factors that influenced their development, and the strategies they used to direct it. To date, little research of this kind has been conducted in forensic psychiatry. In this study, we used the deliberate practice model of elite performance as a heuristic to interpret the accounts of several experienced and distinguished practitioners, revealing and characterizing the influences and activities they identify as having been most important to their development. Semi-structured telephone interviews were conducted with six participants from across North America who started their forensic careers between 1965 and 1980. Transcripts were analyzed using directed content analysis. Participants cited little in the way of highly structured activities designed specifically to improve performance. They instead described using opportunities to learn from real casework and additional knowledge pursuits, as well as using deliberate career management to structure the conditions of their work-based learning. They also stressed the effect of entering forensic practice during a period of increasing interest, demand and investment, which yielded early opportunities to learn through practice. We discuss limitations in the deliberate practice model's capacity to capture key learning strategies in forensic psychiatry, connections between work-based learning and the discipline's general historical trajectory, and the role of career management in professional development strategies.
Assarroudi A, Heshmati Nabavi F, Armat MR, Ebadi A, Vaismoradi M. Directed qualitative content analysis: the description and elaboration of its underpinning methods and data analysis process. Journal of Research in Nursing. 2018;23(1):42-55. doi:10.1177/1744987117741667.
Ericsson KA, Krampe RT, Tesch-Romer C. The role of deliberate practice in the acquisition of expert performance. Psychol Rev. 1993;100(3):363-406. doi.org/10.1037/0033-295X.100.3.363
Gardner H. Why would anyone become an expert? Am Psychol. 1995;50(9):802-803. doi.org/10.1037/0003-066X.50.9.802
Macnamara BN, Hambrick DZ, Oswald FL. Deliberate practice and performance in music, games, sports, education, and professions: a meta-analysis. Psychol Sci. 2014;25(8):1608-1618. doi: 10.1177/0956797614535810
Berliner DC. Learning about and learning from expert teachers. International Journal of Educational Research. 2001;35(5):463-482.
van de Wiel MW, Van den Bossche P, Janssen S, Jossberger H. Exploring deliberate practice in medicine: How do physicians learn in the workplace? Adv Health Sci Educ Theory Pract. 2001 Mar;16(1):81-95. doi: 10.1007/s10459-010-9246-3
Glancy GD. The case for progress in forensic psychiatry. J Am Acad Psychiatry Law. 2020 Mar;48(1),7-11. doi: 10.29158/JAAPL.003908-20
Booth B, Chatterjee S, Watts J, Glancy G. Towards a new model of training in Canadian forensic psychiatry. J Am Acad Psychiatry Law 49:In Press, 2021. DOI:10.29158/JAAPL.200112-20.
Glancy, G., & Miller, D. (2021). The Greats: Learning Strategies of Master Forensic Psychiatrists. International Journal of Risk and Recovery, 4(1), 43–50. https://doi.org/10.15173/ijrr.v4i1.3911
Copyright (c) 2021 Daniel Miller, Graham Glancy
Authors retain copyright of their work and grant the International Journal of Risk and Recovery the right of first publication with the work simultaneously licensed under a Creative Commons Attribution License. This allows others to share the work with an acknowledgement of the work's authorship and initial publication in this journal.
Authors are able to enter into separate, additional contractual arrangements for the non-exclusive distribution of the journal's published version of the work (e.g., post it to an institutional repository or publish it in a book) with an acknowledgement of its initial publication in this journal.
Authors are permitted and encouraged to post their work online (e.g., in institutional repositories or on their websites) before and during the submission process as it can lead to productive exchanges, as well as earlier and greater citation of published work. (See The Effect of Open Access.)
Graham Glancy, Marissa Heintzman, Adam Wheeler, Battered woman syndrome , International Journal of Risk and Recovery: Vol. 2 No. 2 (2019)
Aisha Christiansen, Jodi L. Viljoen, Erin K. Fuller, Examination of the Structured Assessment of Protective Factors for Violence Risk - Youth Version (SAPROF-YV) in Canadian Adolescents , International Journal of Risk and Recovery: Vol. 4 No. 2 (2021)


The Life of a Truly Free Person – Wake Up and Laugh!
For a wet Wednesday afternoon, here's a poem by Daehaeng Kun Sunim that's also used as a song. These songs are so good! lol. They just blow me away.
taking a drink of clear water.
to hold them all steady.
than this life of a free person?
and the heavens begin to rotate around this pillar.
is every being in the universe.
this life of a truly awakened one.