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Enhanced Measurement-Based care Effectiveness for Depression (EMBED): A Canada-China implementation project
Mood Disorder Centre researchers have been awarded a 5-year CIHR grant to improve depression treatment outcomes in Shanghai using novel tech tools.
We are excited to announce the Canadian Institutes of Health Research (CIHR) and National Natural Science Foundation of China (NSFC) through the Global Alliance for Chronic Diseases (GACD) have awarded a team of Mood Disorders Centre and other researchers approximately $2.1 million over 5 years to conduct a research and implementation program to improve depression treatment and outcomes in China.
The project, called "Enhanced Measurement-Based care Effectiveness for Depression" (EMBED), will adapt and develop technologies such as mobile apps, online training programs, electronic medical records, and internet, telephone and WeChat interventions to promote measurement-based care (MBC) for depression in community mental health centres across Shanghai. MBC is an evidence-based practice that can improve depression diagnosis and treatment, and technology-enabled MBC (called "enhanced" or eMBC) tools developed through the program may serve as models for future development and scale up in the region.
Principal Investigators are Dr. Raymond Lam, Professor of Psychiatry at the University of British Columbia (UBC) and Director of the Mood Disorders Centre (Canada) and Dr. Chen Jun, Professor of Psychiatry at the Shanghai Jiao Tong University (China) and Director of the Clinical Research Center at the Shanghai Mental Health Centre.
Dr. Erin Michalak, Professor in the Department of Psychiatry at UBC and a research psychologist of the Mood Disorders Centre, is also a Co-Investigator on the project. Dr. Jill Murphy is a Postdoctoral Fellow for EMBED, funded by a MITACS Elevate Award.
The program is also one of the first initiatives affiliated with the Asia-Pacific Economic Cooperation's (APEC) Digital Hub for Mental Health, which supports APEC's vision to strengthen mental health and reduce the economic impact of mental illness in the Asia-Pacific region.
Read the press release (2017)
Read the CBC news article. (Nov, 2017)
See the summary of progress video, presented at the 2018 GACD Annual Scientific Meeting in Sao Paulo, Brazil, November 2018.
Our first EMBED publication is now available from Global Mental Health – free open access!
Murphy JK, Michalak EE, Colquhoun H, Woo C, Ng CH, Parikh SV, Culpepper L, Dewa CS, Greenshaw AJ, He Y, Kennedy SH, Li XM, Liu T, Soares CN, Wang Z, Xu Y, Chen J, Lam RW. Methodological approaches to situational analysis in global mental health: a scoping review. Glob Ment Health (Camb). 2019 Jun 13;6:e11.
Grant details:
Grant Title: Enhanced Measurement-Based Care Effectiveness for Depression (EMBED): A Canada-China Implementation Project
Funding Amount: 2.1 million over 5 years
Funding Agencies: Canadian Institutes of Health Research (CIHR) Roadmap Accelerator Fund (RAF) in partnership with the National Natural Science Foundation of China (NSFC)
Investigators:
Principal Investigator, Canada:
Dr. Raymond W. LAM, MD, FRCPC
Professor and BC Leadership Chair in Depression Research;
Associate Head for Research and International Affairs, Department of Psychiatry, University of British Columbia;
Director, Mood Disorders Centre, Djavad Mowafaghian Centre for Brain Health;
Principal Investigator, China:
Dr. Jun CHEN, MD, PhD
Director & Chief Physician, Depressive Disorders Program, Division of Mood Disorders
Director, Office of Clinical Research Center
Director, Office of Shanghai Clinical Center for Mental Disorders
Shanghai Mental Health Center, Shanghai Jiao Tong University School of Medicine (SMHC)
Dr. Heather COLQUHOUN University of Toronto
Dr. Larry CULPEPPER Boston University
Dr. Carolyn DEWA University of California, Davis
Dr. Andrew GREENSHAW University of Alberta
Dr. Yanling HE Shanghai CDC for Mental Health
Dr. Sidney KENNEDY University of Toronto
Dr. Xin-Min LI University of Alberta
Dr. TianLi LIU Peking University
Dr. Erin MICHALAK University of British Columbia
Dr. Jill MURPHY University of British Columbia
Dr. Chee NG University of Melbourne, Australia
Dr. Sagar PARIKH University of Michigan, Ann Arbor
Dr. Claudio SOARES Queen's University
Mr. Phil UPSHALL Mood Disorders Society of Canada
Dr. Zuowei WANG Shanghai Mental Health Center/Hongkou District Mental Health Center of Shanghai, Shanghai JiaoTong University School of Medicine
Dr. Yifeng XU Shanghai Mental Health Center, Shanghai Jiao Tong University School of Medicine (SMHC)
Depression affects 300+ million people globally and is now the leading cause of disability and burden of disease worldwide. In China, the National Mental Health Work Plan 2015-20 specifies improving the ability of healthcare facilities to identify depression and increase the treatment rate by 50%. Measurement-based care (MBC) – the routine use of validated outcomes such as the PHQ-9 depression questionnaire to guide clinical decision-making – is a simple evidence-based practice (EBP) that may help meet these objectives. However, there is still a significant care gap in the implementation of MBC in China and elsewhere. In Canada, we have adopted the concept of enhanced MBC (eMBC), in which technology can engage both patients & physicians in using MBC; eMBC enhancements include internet and mobile app tools for patients to track their own progress with the PHQ-9, and an evidence-based, low-cost, low-intensity psychological treatment (computer/internet guided self-management with telephone/WeChat lay coaches) that has embedded patient measurement and feedback to physicians.
EMBED: a Canada-China implementation project, proposes to develop a novel EBP implementation strategy by adapting, implementing and evaluating eMBC in diverse community mental health clinics in Shanghai, modeled on programs implemented in Canada. EMBED addresses 4 broad aims: 1) identify contextual enablers & barriers to MBC implementation; 2) explore physician- and patient-level factors as mediators for an EBP implementation; 3) provide clinical & health economic outcomes to establish effectiveness of eMBC; and 4) build knowledge & capacity for scale up of eMBC in China and beyond. Our hypothesis is that physician & patient factors that are barriers for implementation of standard MBC will be enablers for implementation of eMBC.
To achieve these aims, we will first conduct a Situational Analysis to determine the key barriers & enablers for MBC implementation in Shanghai. We will adapt a Canadian eMBC program for the Chinese context, then will use a hybrid implementation-effectiveness design (an adaptive cluster randomized evaluation) to compare eMBC with standard MBC implementation in 12 community clinics, 240 physicians, and 1200 patients. We hypothesize that eMBC implementation will lead to superior implementation, patient and cost-effectiveness outcomes, compared to standard MBC.
EMBED will advance the international literature on MBC broadly by focusing on the understudied role of patients in implementation of MBC. EMBED will also further implementation science by creating new knowledge on contextual factors, including mediating effects of physician- and patient-level factors, together, on EBP implementation outcomes. Moreover, the unique partnership of the EMBED team with the APEC Digital Hub for Mental Health will ensure a pathway for integrated knowledge & policy translation so that findings will have significant scale-up and spread potential in other regions in China, the Asia-Pacific and worldwide.
Last updated on September 18, 2019 @3:17 pm


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Migration and Inequality A Structural Approach
Migration, immigrants, inequality, structures, incorporation, equity
Ron Hayduk
Migrants are omnipresent in cosmopolitan societies. Propelled from their homelands by poverty, violence, and environmental disasters—and the promise of better opportunities and security—migrants have found their way into metropolitan regions. At the same time, we see steep increases in economic inequality. These changes, which are intrinsically connected to the rise of neoliberal polices, have pushed immigration to the top of the political agenda for both the political right and left in many nations. The right seeks to erect walls, restrict immigration, and deport the undocumented. The left seeks amnesty, sanctuary policies and other measures to advance human rights in response to the migration crisis. Yet neither approach addresses the underlying causes of migration nor growing inequalities that together animate populist revolts on both the left and right across the globe.
In this paper, I employ a framework that foregrounds capitalist accumulation at the center of these processes. Focusing on urban areas in the US, I highlight the ways economic, social and political structures contribute to growing inequalities between immigrants and the native born -- as well as sharp inequalities within each group -- which, in turn, affect patterns of immigrant incorporation, politics and options for reform. The paper examines US immigration and immigrant policy, assessing their impacts on inequality and immigrant incorporation processes and outcomes. I conclude by pointing to contemporary social movements and evolving political alignments, which have the potential to achieve more egalitarian outcomes capable of sustaining social cohesion in metropolitan regions, as well as more stable and robust democratic systems across borders. Given that immigrants and their offspring comprise nearly one in four people in the U.S., addressing such inequalities is theoretically important and a pressing political concern.
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Bacon, David. 2013. The right to stay home: How US policy drives Mexican migration. Beacon Press.
Stanley-Becker, Tom, "Strange Bedfellows: Business, Labor, Guest Workers, and Immigration Reform in the United States, 1986-2013" (2013). Harvey M. Applebaum '59 Award. 5.
http://elischolar.library.yale.edu/applebaum_award/5
Card, David, and Steven Raphael, eds. (2013). Immigration, poverty, and socioeconomic inequality. Russell Sage Foundation.
Chishti, Muzaffar and Jessica Bolter. 2019. "Merit-Based" Immigration: Trump Proposal Would Dramatically Revamp Immigrant Selection Criteria." Migration Policy Institute. MAY 30, 2019. https://www.migrationpolicy.org/article/merit-based-immigration-trump-proposal-immigrant-selection
Colbern, A., & Karthick Ramakrishnan, S. (2018). Citizens of California: How the golden state went from worst to first on immigrant rights. New Political Science, 40(2), 353-367.
de Graauw, Els. 2016. Making immigrant rights real: Nonprofits and the politics of integration in San Francisco. Cornell University Press.
de Souza Briggs, Xavier. 2013. "Conclusion rethinking immigrant political incorporation." Outsiders No More?: Models of Immigrant Political Incorporation 321.
Durand, Jorge, and Douglas S. Massey. (2019). "Evolution of the Mexico-US Migration System: Insights from the Mexican Migration Project." The ANNALS of the American Academy of Political and Social Science 684, no. 1: 21-42.
Farber, Henry S. Daniel Herbst, Ilyana Kuziemko, Suresh Naidu. "Unions and Inequality Over the Twentieth Century: New Evidence from Survey Data". WORKING PAPER #620, PRINCETON UNIVERSITY, INDUSTRIAL RELATIONS SECTION. May 2, 2018. http://arks.princeton.edu/ark:/88435/dsp01gx41mm54w
Fletcher Jr., Bill and Fernando Gapasin. (2008). Solidarity Divided: The Crisis in Organized Labor and a New Path toward Social Justice. Berkeley: University of California Press.
Freeman, Gary P., David L. Leal, and Jake Onyett. (2013). "Pointless: On the failure to adopt an immigration points system in the United States." In Wanted and Welcome? pp. 123-143. Springer, New York, NY.
Gordon, Colin. (2013). "Growing apart: A political history of American inequality." Accessed December 19.
Guglielmo, Thomas. (2003). White on Arrival: Italians, Race, Color, and Power in Chicago, 1890–1945 (New York, NY: Oxford University Press.
Guskin, Jane and David Wilson. 2017. The politics of immigration: Questions and answers. NYU Press.
Hayduk, Ron and Susanna Jones. (2008). "Immigrants and Race in the US: Are Class-Based Alliances Possible?" Socialism and Democracy. Vol 22, Issue No. 3. pp 75-95.
Hayduk, Ron and Marcela García-Castañon. 2018. Symposium and Introduction: "Xenophobia, Belonging and Agency: Citizenship in Immigrant America." New Political Science. Vol. 40, No. 2
Hero, Rodney. (2003). "Multiple theoretical traditions in American politics and racial policy inequality." Political Research Quarterly 56, no. 4: 401-408.
Hsin, Amy. (2016.) "How Selective Migration Enables Class Mobility." Ethnic and Racial Studies 39(13): 2379- 2384.
Hochschild, Jennifer, Jacqueline Chattopadhyay, Claudine Gay, and Michael Jones-Correa. eds. (2013). Outsiders No More? Models of Immigrant Political Incorporation. (London: Oxford University Press).
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Kauffman, L.A. 2018(b) "We are living through a golden age of protest." May 6, 2018. The Guardian. https://www.theguardian.com/commentisfree/2018/may/06/protest-trump-direct-action-activism
Kochhar, Rakesh and Anthony Cilluffo. (July 12, 2018). "Income Inequality in the U.S. Is Rising Most Rapidly Among Asians: Asians displace blacks as the most economically divided group in the U.S." Pew Research Center. https://www.pewsocialtrends.org/2018/07/12/income-inequality-in-the-u-s-is-rising-most-rapidly-among-asians/
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redpajama_set_name: RedPajamaCommonCrawl


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Home / Safety / Canadian Air Force grounds Snowbirds aerobatic team
Canadian Air Force grounds Snowbirds aerobatic team
Blog Before Flight Staff August 12, 2022 0
RCAF Snowbirds aerobatic team.
The Government of Canada announced yesterday that following the accident involving a 431 (Air Demonstration) Squadron CT-114 Tutor aircraft on August 2, 2022 in Fort St. John, B.C. the Commander of 1 Canadian Air Division has ordered an operational pause on the CT-114 fleet.
As the Operational Airworthiness Authority for the Royal Canadian Air Force (RCAF), Major General Iain Huddleston implemented the operational pause after consulting with Directorate of Flight Safety investigators and with experts from the Technical Airworthiness Authority within the Department of National Defence's Assistant Deputy Minister (Materiel).
"Royal Canadian Air Force aircraft cannot be flown unless they are determined to be airworthy and safe to fly. Given that the cause of this accident remains to be determined by the Airworthiness Investigative Authority, I have ordered an operational pause on the CT-114 Tutor fleet as we continue the investigation and commence a thorough operational airworthiness risk assessment process. We will return the fleet to flying operations when it is safe to do so, and in accordance with our rigorous airworthiness program," Huddleston said.
The RCAF will conduct a deliberate, detailed and broad risk analysis, with the aim of enabling the safe resumption of CT-114 flying operations. This operational pause means the fleet of aircraft will not fly until an operational airworthiness risk assessment can be completed.
The RCAF's airworthiness system will assess whether the accident and its causes pose any risk to continued flying operations, and if so, what mitigation measures can but put in place to lower those risks. The cause of the accident remains under investigation by the Royal Canadian Air Force's Directorate of Flight Safety.
On August 2, a CT-114 Tutor aircraft of 431 (Air Demonstration) Squadron experienced an emergency during takeoff in Fort St. John, B.C. The pilot, who was sole occupant, was able to land the plane immediately, but the plane was damaged in the process. The pilot was medically assessed and was uninjured. An investigation into the accident by the RCAF's Directorate of Flight Safety is currently underway.
The RCAF has an active fleet of 20 CT-114 Tutor aircraft, operated by 431 (AD) Squadron based at 15 Wing Moose Jaw.
The CT-114 Tutor is flown exclusively by Canadian Forces Snowbirds air demonstration team at public events throughout North America. The Snowbirds showcase the high level of skill, professionalism and teamwork, inherent in the members of the Canadian Armed Forces.
The Tutor aircraft was a primary trainer for the Royal Canadian Air Force until 2000. The Tutors flown by the Snowbirds are slightly modified for show features and enhanced performance during low-level aerobatic flying.
👉 You may also like: No replacement for RCAF Snowbirds, the Tutor to be kept until 2030
Source: Government of Canada


The HP Pavilion ze5000 is the general name for a number of variants for the device that all operate the same but differ aesthetically, such as the ze5270 or ze5250. First released in late 2000 and variants released throughout 2003, the devices all share the same general setup and operations.
The HP Pavilion ze5000, made by Hewlett-Packard, is the the successor to the xe4500 adding a faster processor and a larger hard drive to the nine pound frame. The ze5000 is the title for a series of laptops that were released starting in 2002 and went into 2003. Some variations include the ze5270 and the ze5250. All of these are the same structurally, and will only alternate their appearance. In order to detect which version you have, you can simply check the underside of your device for a small white tag with black lettering denoting the series title (Ze) followed by a four digit series of numbers, starting with 5. A fair price coupled with these much needed upgrades allowed for the ze5000 to be on the top competing tier when it was released in 2002. The ze5000 was one of the earliest laptops to utilize the screen mirroring technology with the use of an S-Video plug. Accompanying the 15 inch screen and sixty gigabyte hard drive is the 2.8 GHz pentium 4 processor, one of the most pristine on the market at the time. The device's keyboard is quiet and firm with 19.22 mm long keys embedded 2.3 mm deep into the chassis. Located at the top of the keyboard are the Five-application launch startup buttons for easy task managing and integration when mirrored onto the big screen. Sound quality was ensured with the Altec Lansing speakers allowing for top quality audio without notable distortion.


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\section{Introduction}
In higher dimensions a true crystal, named Wigner crystal, where the density is perfectly ordered, is possible when the repulsion between particles dominates over the kinetic energy in the case of small density. In one dimension, quantum fluctuations prevent any type of true spin-symmetry breaking and long-range order in the ground state, and thus the crystal does not have perfect order~\cite{ref:giamarchi_book,Schulz,Wigner}. However, in one dimension, the equilibrium positions of the electrons are
assumed to be equally spaced and a solid like state can be produced when the correlation length exceeds the sample length~\cite{ref:Mueller}. The liquid-to-quasi-Wigner crystal crossover when the density decreasing can be characterized by the onset of the $4k_F$-peak in the static structure factor following from the Luttinger liquid predictions~\cite{Schulz, ref:Shulenburger}, with $k_{\rm F}$ the Fermi wave vector (related to the fermion density $n$ by $k_{\rm F}=\pi n/2$), or by the $N_f-1$ high-contrast peaks in the pair correlation function~\cite{ref:Wang}, with $N_f$ the particle number in the system.

In the system where the constituent particles are not electrons but dilute atoms, the fundamental interaction is no longer
of long-range Coulomb type but of short-range contact one, which is the case in the field of ultracold atomic systems.
In this system, the ground-state density profile displays at strong coupling well-pronounced Wigner oscillations with a `$4k_{\rm F}$ periodicity'. However, the static structure factor or the pair correlation function does not show any signature of Wigner-molecule-type correlations like that in the system of long-range interaction~\cite{Astrakharchik0},
which means Wigner-type molecules are absent in the system of short-range interaction~\cite{ref:Wang}. In this paper, we focus only on the ``$2k_F\rightarrow 4k_F$ crossover" in the density profiles: for vanishing and weak interactions the ground state is liquid-like with $2k_{\rm F}$-Friedel oscillations, whereas at strong repulsions a periodicity of $4 k_{\rm F}$-Wigner oscillation emerges.

For the one-dimensional (1D) harmonically trapped system of spin-balanced or imbalanced fermionic atomic gases, many numerical schemes have been used in studying lots of interesting quantum effects~\cite{Machida,Molina,Rigol,Astrakhardik,Casula,exact diagonalization,Nikkarila}.
A density-functional scheme using as reference the Bethe-ansatz solvable homogeneous system was proposed to calculate the ground-state properties~\cite{ref:burke,ref:gao_pra_2006}. However, this approach was found to fail at the strong-coupling limit~\cite{ref:gao_pra_2006}. More precisely, the exchange-correlation potential proposed there is not able to describe the $2k_{\rm F}\rightarrow 4k_{\rm F}$ crossover, which, as noted above, is expected to occur upon increasing the strength of the repulsive interactions between antiparallel-spin particles.

A simple functional is proposed in Ref.~[\onlinecite{ref:saeed_pra_2007}] for a two-particle system that embodies this crossover and is capable of describing inhomogeneous Luttinger liquids with strong repulsions. The main idea is to capture the tendency to $4k_F$-Wigner oscillations by adding an infinitesimal spin-symmetry-breaking magnetic field to the Hamiltonian and by resorting to spin-density functional theory (SDFT) based on the spin-polarized Bethe-ansatz equations~\cite{ref:Capelle,ref:gaoAsgari}.

For fermions loaded in a 1D optical lattice, the system can be modeled by a 1D Fermi-Hubbard model.
Friedel oscillations of wavelength $2k_{\rm F}$ and $4k_{\rm F}$ component are analyzed in this model with open boundary condition by both the Bethe-ansatz based SDFT, the exact diagonalization~\cite{ref:Vieira}, bosonization, and numerical density matrix renormalization group calculations~\cite{1D_wigner_HM,soffing_pra_2011,ref:Bedurftig}. It was found that the $2k_{\rm F}\rightarrow 4k_{\rm F}$ crossover takes place at $U=4t$. For an unpolarized system, if a tiny magnetization which is proportional to the difference of the spin-up and spin-down densities is induced by hand into the exchange-correlation potential, the $4k_F$-oscillation appears in the density profile at the expense of violating the Lieb-Mattis theorem, while for a polarized system, SDFT can reproduce both the $2k_{\rm F}$ and $4k_{\rm F}$ oscillations without violating the Lieb-Mattis theorem~\cite{ref:Vieira}. It is found that the $4k_F$ density oscillations is strongly related to the large Fermi sea induced by the strong repulsion between different spin species~\cite{1D_wigner_HM,soffing_pra_2011}.

Some 1D systems, for example, the 1D Gaudin-Yang gas in a homogeneous continuum space, or the 1D Lieb-Wu model of particles in a discrete lattice, i.e., 1D Fermi-Hubbard model, where the fermions interact through attractive or repulsive short-range interactions, are exactly solvable. However, in the inhomogeneous case only some special systems can be solved exactly. For example, the 1D two-component Fermi gas in an infinite potential well can be solved exactly by the Bethe-ansatz techniques, where the ground state properties are investigated~\cite{ref:Wei}.
The density profiles are evaluated from weak to very strong interactions. In the strongly interacting limit, the density profile tends to that of the spinless fermions though the momentum distributions differ. An exact analytical solution of 1D spin-1/2 fermions with infinite repulsion for arbitrary confining potential is obtained by the combination of Girardeau's hard-core contacting boundary condition and group theoretical method~\cite{ref:Guan}. For the spin-imbalanced case they found that the spin-up and spin-down density distributions show alternative peaks avoiding overlapping together and the parity symmetry.

In this paper, we will employ the Bethe-ansatz based SDFT to investigate the 1D inhomogeneous system with general interaction strengths. Our results are compared against the above mentioned exact analytic and the exact numerical diagonalization method. The Wigner oscillations while increasing coupling strength for both unpolarized and polarized cases will be studied.

The rest of the paper is organized as follows. In Sec. II, we present the model and the method. The numerical results are followed in Sec. III. In Sec. IV, we conclude what we found.

\section{Model and the method}
In this work we consider a 1D system of two-component Fermi gas with a contact repulsive interaction of strength $g_{\rm 1D}$~\cite{ref:olshanii_1998}.
The two fermion species are taken to have the same mass $m$, with $N_\uparrow$ spin-up species and $N_\downarrow$ spin-down ones. The total number of particles is $N_f=N_\uparrow+N_\downarrow$. The system is described by the Hamiltonian,
\begin{equation}\label{eq:igy}
{\cal H}=-\frac{\hbar^2}{2m}\sum_{i=1}^{N_f}\frac{\partial^2}{\partial z^2_i}+g_{\rm 1D}\sum_{i=1}^{N_{\uparrow}}\sum_{j=1}^{N_{\downarrow}}\delta(z_i-z_j)+V_{\rm ext}\,,
\end{equation}
where contact interactions between parallel-spin particles are suppressed by the Pauli exclusion principle and $V_{\rm ext}$ the confining potential. We consider that the atoms are either confined in a 1D box of length $L$ ($V_{\rm ext}=0$ inside the box and $V_{\rm ext}=+\infty$ elsewhere) or subjected to a strongly anisotropic harmonic potential $V_{\rm ext}=\sum_{i=1}^{N} V_{\rm ext}(z_i)=(m\omega^2_{\|}/2)\sum_{i=1}^{N}z^2_i$, characterized by angular frequencies $\omega_\perp$ and $\omega_\|$ in the radial and axial directions with $\omega_\| \ll \omega_\perp$. For the system of harmonic trap,
we choose the harmonic-oscillator length $a_{\|}=\sqrt{\hbar/(m\omega_{\|})}$ as unit of length and the harmonic-oscillator quantum $\hbar\omega_{\|}$ as unit of energy.
The Hamiltonian (\ref{eq:igy}) can be shown to be governed by the dimensionless coupling parameter
\begin{equation}\label{eq:lambda}
\lambda=\frac{g_{\rm 1D}}{a_{\|}\hbar\omega_{\|}}\,.
\end{equation}
For $V_{\rm ext}=0$ the Hamiltonian (\ref{eq:igy}) reduces to the homogeneous Gaudin-Yang model solvable by means of the Bethe-ansatz technique~\cite{ref:GY} and determined by
the linear density $n=N/L$, by the spin polarization $\zeta=(N_{\uparrow}-N_{\downarrow})/N$, and by the interaction strength $g_{\rm 1D}$.
\begin{figure}
\begin{center}
\includegraphics[width=1.00\linewidth]{Fig1.eps}
\caption{(Color online) The ground-state density distributions as a function of $z/a_{||}$ for a balanced Fermi gas with $N_\uparrow=N_\downarrow=5$
confined in a harmonic trap for various interaction strengths. The crossover from $2k_F$- to $4k_F$-oscillations with increasing
interaction strength $\lambda$ is showed by the doubling of the crests in the density profile.
The dominance of the $4k_F$-oscillations over $2k_F$-ones can be better evidenced by the density derivative $dn(z)/dz$.
In the inset, the derivative of the density with respect to $z$ is shown for $\lambda=1, 6$, and $8$ as an indicator to examine the $2k_{\rm F}\rightarrow 4k_{\rm F}$ crossover.
\label{fig:one}}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\includegraphics[width=1.00\linewidth]{Fig2.eps}
\caption{(Color online) The ground-state density distributions (in arbitrary length$^{-1}$ unit) as a function of $z$ (in arbitrary length unit) for a polarized Fermi gas with $N_\uparrow=2$ and $N_\downarrow=1$
confined in a box of length $L=1$ for various interaction strengths. The SDFT results are plotted in symbols and the exact Bethe-ansatz ones in (colored) lines. The thin (black) solid line represents the result in the infinite repulsive interaction limit.
\label{fig:three}}
\end{center}
\end{figure}

The ground-state spin-density distributions $n_\sigma(z)$ can be calculated within SDFT by solving self-consistently the Kohn-Sham (KS) equation,
\begin{equation}\label{eq:kss}
\left[-\frac{\hbar^2}{2m}\frac{\partial^2}{\partial z^2}+V^{(\sigma)}_{\rm KS}[n_\sigma](z)\right]\varphi_{\alpha,\sigma}(z)=\varepsilon_{\alpha,\sigma}\varphi_{\alpha,\sigma}(z)
\end{equation}
together with the closure
\begin{equation}\label{eq:closure}
n_\sigma(z)=\sum_{\alpha=1}^{N_\sigma}\left|\varphi_{\alpha,\sigma}(z)\right|^2\,.
\end{equation}
Here, $V^{(\sigma)}_{\rm KS}[n_\sigma](z)=V^{(\sigma)}_{\rm H}[n_\sigma](z)+V^{(\sigma)}_{\rm xc}[n_\sigma](z)+V_{\rm ext}(z)$ is the spin-dependent effective KS potential.
The first term in $V^{(\sigma)}_{\rm KS}$ is the mean-field term $V^{(\sigma)}_{\rm H}=g_{\rm 1D}n_{\bar \sigma}(z)$, while the second term is the exchange-correlation potential defined as the functional derivative of the exchange-correlation energy $E_{\rm xc}[n_\sigma]$ evaluated at the ground-state density profile, $V^{(\sigma)}_{\rm xc}=\delta E_{\rm xc}[n_\sigma]/\delta n_\sigma(z)|_{\rm \scriptscriptstyle GS}$.

To obtain the density distribution $n_\sigma(z)$ from Eqs.~(\ref{eq:kss}) and~(\ref{eq:closure}), approximations to the exchange-correlation functions $E_{\rm xc}$ are unavoidable. The local-spin-density approximation (LSDA) is known to provide an excellent description of the ground-state properties of a variety of inhomogeneous systems~\cite{ref:Giuliani_and_Vignale}. In the following we employ a Bethe-ansatz-based LSDA (BALSDA) functional for the exchange-correlation potential,
\begin{eqnarray}\label{eq:balda}
E_{\rm xc}[n_\sigma] & \rightarrow & E^{\rm LSDA}_{\rm xc}[n_\sigma]\\
&=&\int dz\, n(z)\left.\varepsilon^{\rm hom}_{\rm xc}(n,\zeta,g_{\rm 1D})\right|_{n\rightarrow n(z),\zeta\rightarrow \zeta(z)}\,,\nonumber
\end{eqnarray}
where the exchange-correlation energy $\varepsilon^{\rm hom}_{\rm xc}$ of the homogeneous Gaudin-Yang model is defined by
\begin{eqnarray}\label{eq:xc}
\varepsilon^{\rm hom}_{\rm xc}(n,\zeta,g_{\rm 1D})&=&\varepsilon_{\rm GS}(n,\zeta,g_{\rm 1D})-\kappa(n,\zeta)\nonumber\\
&-&\varepsilon_{\rm H}(n,\zeta,g_{\rm 1D})\,.
\end{eqnarray}
Here $\varepsilon_{\rm GS}(n,\zeta,g_{\rm 1D})$ is the ground-state energy of the exact Bethe-ansatz solution of the model,
$
\varepsilon_{\rm H}(n,\zeta,g_{\rm 1D})=\frac{1}{4}g_{\rm 1D}n^2(1-\zeta^2)
$
is the mean-field energy, and
$\kappa(n,\zeta)=\pi^2\hbar^2 n^2(1+3\zeta^2)/24m$ is the noninteracting kinetic energy~\cite{ref:GY}.
\begin{figure*}
\begin{center}
\tabcolsep=0 cm
\begin{tabular}{cc}
\scalebox{0.35}[0.35]{\includegraphics{Fig3a.eps}}&
\scalebox{0.35}[0.35]{\includegraphics{Fig3b.eps}}\\
\scalebox{0.35}[0.35]{\includegraphics{Fig3c.eps}}&
\scalebox{0.35}[0.35]{\includegraphics{Fig3d.eps}}
\end{tabular}
\caption{(Color online) The ground-state density distributions as a function of $z/a_{||}$ for a polarized Fermi gas with $N_\uparrow=2$ and $N_\downarrow=1$
confined in a harmonic trap ranges from weak to strong interaction strengths: (a) $\lambda=1$; (b) $\lambda=5$; (c) $\lambda=8$; (d) $\lambda=15$. The SDFT results are plotted in symbols ($\color{red}\circ$, $ \color{green}\bullet$, and $\color{blue}\triangle$, respectively, for $n$, $n_\uparrow$, and $n_\downarrow$ ) and the exact diagonalization ones in lines.
\label{fig:four}}
\end{center}
\end{figure*}
\begin{figure}
\begin{center}
\tabcolsep=0 cm
\includegraphics[width=1.00\linewidth]{Fig4.eps}
\caption{(Color online) The 3D plot of the ground-state density distributions as a function of the dimensionless interaction strength $\lambda$ and $z/a_{||}$ for a polarized Fermi gas with $N_\uparrow=2$ and $N_\downarrow=1$
confined in a harmonic trap. The results are obtained based on the SDFT.
\label{fig:five}}
\end{center}
\end{figure}

\section{Numerical results}
In this section, we present our numerical results by employing the Bethe-ansatz based SDFT to investigate the 1D inhomogeneous system with broad interaction strengths. Our results are compared against the exact numerical diagonalization method while this method is available when the system is small. For the polarized system in a box, we compare our results with the analytical ones which are available in this case by the exact Bethe-ansatz method.

\subsection{Unpolarized system confined in a trap}
In Fig. \ref{fig:one}, we study an unpolarized Fermi gas with the number of total particles $N_f=10$
confined in a harmonic trap. The ground-state density distributions is calculated for various interaction strengths within SDFT.
For the unpolarized system, the KS equations have to be solved self-consistently by taking one of the following methods to obtain
the correct $2k_{\rm F}\rightarrow 4k_{\rm F}$ crossover. (i) One can either add an infinitesimal spin-symmetry-breaking magnetic field.
The field strength is infinitesimal small and reduced to zero during the self-consistent solution of the KS equations. (ii)
Alternatively one can solve the KS equations from an initial guess which has slightly broken spin symmetry [{\it i.e.} an initial guess with  $n_\uparrow(z)\neq n_\downarrow(z)$], without using any $B$ field, (iii) The last possibility is to break the symmetries of the density distributions just one time by shifting the center of the densities during the self-consistent cycle [for example, let $n_\uparrow(z)= n_\uparrow(z+b)$ with $b$ a nonzero value].
When $\lambda$ is small, the above mentioned methods restore the results from the Bethe-ansatz based local density approximation (BALDA)~\cite{ref:Capelle}.
However when $\lambda$ is large, the final result for the total density $n(z)$ from the BALSDA is very different from that resulting from the BALDA theory~\cite{ref:gao_pra_2006}. We want to mention here that, without using the above mentioned symmetry-breaking procedure, the BALSDA theory produces the same results as that of BALDA. That is, for the BALSDA theory, to achieve a correct shape for the density profile, one has to use one of the (i)-(iii) procedure~\cite{ref:saeed_pra_2007}. This method has long been used in the literature in discussing the ground-state of the $H_2$ molecule at any bond length. The symmetry-breaking choice typically produce a spin-unpolarized density out to a critical bond length by localizing an up-spin electron on one nucleus and a down-spin electron on the other. While this leads to an incorrect spin-density, but it leads to the correct dissociation limit for the energy and the correct total density~\cite{Gunnarsson0}.

At the weak interaction regime, the density is characterized by $2k_F$-Friedel oscillations with $N_f/2$ peaks.
As the interaction strength increases to the strongly interacting limit, the number of peaks in the density profile is doubled. The atoms are distributed in order to minimize the interparticle repulsion energy. This leads to the emergence of $N_f$ crests in the density profile characterized by strong correlations and the $4k_F$-Wigner oscillations. In this case the atoms behave like a fully polarized (or noninteracting spinless) fermions as in the Tonks-Girardeau gas~\cite{ref:hard-core boson}.
Numerically we find that a crossover from the $2k_F$-Friedel oscillations of $N_f/2$ peaks to the $4k_F$-Wigner oscillations happens around $\lambda=6.2$ accompanied of $N_f$ peaks. The crossover is smooth, see, for example, the extensive density-matrix renormalization group study by S\"{o}ffing {\it et al.}~\cite{1D_wigner_HM,soffing_pra_2011}. In the inset, a derivative of the density with respect to $z/a_{\|}$ is used as an indicator to signal the $2k_{\rm F}\rightarrow 4k_{\rm F}$ crossover. We find more clearly that $N_f$ peaks appear after the threshold value.

\begin{figure}
\begin{center}
\includegraphics[width=1.00\linewidth]{Fig5.eps}
\caption{(Color online) The 3D plot of the ground-state density distributions as a function of the dimensionless interaction strength
$\lambda$ and $z/a_{||}$ for a polarized Fermi gas with $N_\uparrow=3$ and $N_\downarrow=2$
confined in a harmonic trap. The results are obtained based on the SDFT.
\label{fig:six}}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\includegraphics[width=1.00\linewidth]{Fig6.eps}
\caption{(Color online) The 2D contour plot of the ground-state density distributions as a function of the dimensionless interaction strength
$\lambda$ and $z/a_{||}$ for a polarized Fermi gas with $N_\uparrow=22$ and $N_\downarrow=18$
confined in a harmonic trap. The results are obtained based on the SDFT.
\label{fig:eight}}
\end{center}
\end{figure}
\begin{figure}
\begin{center}
\includegraphics[width=1.00\linewidth]{Fig7.eps}
\caption{(Color online) The 2D contour plot of the ground-state density distributions as a function of the dimensionless interaction strength
$\lambda$ and $z/a_{||}$ for a polarized Fermi gas with $N_\uparrow=34$ and $N_\downarrow=6$
confined in a harmonic trap. The results are obtained based on the SDFT.
\label{fig:nine}}
\end{center}
\end{figure}
In order to evaluate the credibility of the present method, we compare our results in the following against exact methods
for a polarized system in a box (in \ref{sec1}) and a harmonically confined system
of small number of Fermi atoms (in \ref{sec2}).

\subsection{Polarized system in a box}\label{sec1}

In this section we consider a polarized Fermi gas with $N_\uparrow$ up-spin fermions and $N_\downarrow$ down-spin fermions confined in a box of length $L$, which is exactly solvable by the Bethe-ansatz method~\cite{ref:Wei}. In Fig. \ref{fig:three}, we illustrate the ground-state density distributions as a function of $z$ based on the Bethe-ansatz based SDFT for $N_\uparrow=2$ and $N_\downarrow=1$. $L$ is chosen as units of length.
The interaction strength sets the relative importance of the kinetic energy and the interaction. For weak interaction strength, $2$ peaks appear in the density.
When interaction strength becomes stronger (around $g_{1D}=15$), $3$ peaks emerge. At even stronger interaction strength, exchange is suppressed and the atoms act as though they were noninteracting and spinless in analogy to the case studied for bosons with an infinite contact repulsion~\cite{ref:hard-core boson}. For $g_{1D}=1000$, the infinite repulsive interaction limit is reached, which is compared to the spinless fermions results.
In general, when the interaction strength is large enough, the density $n(z)$ distributes between $N_f$ maxima, which is different from the confined 1D electrons of long-range Coulomb interactions where the density vanishes almost completely between well separated maxima~\cite{ref:Jauregwi,1D_wigner}.
We find, in almost all the range of the interaction strength, SDFT gives good results comparing against the exact Bethe-ansatz ones.
The good agreement may be that the exact exchange-correlation energy of the homogeneous system has almost the same form as that of the inhomogeneous (hard-wall) one which is also integrable.

\subsection{Polarized system confined in a trap}\label{sec2}

Here we report our studies on the ground-state density distributions for a polarized Fermi gas confined in a harmonic trap. The SDFT results are compared against the ones by the exact diagonalization method~\cite{ref:Guan}. In Fig. \ref{fig:four} we plot the density profiles for the system with $N_\uparrow=2$ and $N_\downarrow=1$ for $\lambda=1, 5, 8$, and $15$. We find that for $\lambda < 2$, both the total ground-state densities $n(z)$ and the spin-resolved densities show very good agreement between the SDFT results and the exact diagonalization ones. When $\lambda\gtrsim 2$, SDFT still keeps the overall shape of the total ground-state densities well. However, the respective amplitudes of the spin-up and spin-down density are exaggerated by the SDFT. Even for this weakness, the SDFT can help us qualitatively understand the $2k_{\rm F}\rightarrow 4k_{\rm F}$ crossover.
For weak interaction strength, the interaction term gives smaller contribution comparing to the kinetic term, such that $n(z)$ is
dominated by the lowest occupied single-particle states. For the system we studied here, one flat peak is found (See Fig. \ref{fig:four}(a) and (b)).
For strong interaction strength $\lambda\gtrsim 3.8$~\cite{ref:notes}, a structure consisting of $N_f=3$ peaks emerges (See Fig. \ref{fig:four}(c) and (d)), that is, $n(z)$ is signaled in finite region by $N_f=3$ maxima. For even stronger interaction strength $\lambda\gtrsim 15$, the total atom distribution can be described by spinless fermions and the spins tend to decouple with exponentially small exchange interactions. The system degenerates with ferromagnetic and anti-ferromagnetic states~\cite{ref:Guan}.

In Figs. \ref{fig:five} and \ref{fig:six}, the 3D plots of the ground-state density distributions are shown as a function of the dimensionless interaction strength $\lambda$ and $z/a_{||}$. The transition from $2k_{\rm F}$-Friedel oscillations to $4 k_{\rm F}$-Wigner oscillations can be judged by the change in the peaks in the total density distributions, which vary from $1$ to $3$ in Fig. \ref{fig:five} happened at $\lambda\gtrsim 3.8$, and from $3$ to $5$ in Fig. \ref{fig:six} happened at $\lambda\gtrsim 4.7$.

At strongly repulsive limit, the polarized system shows the same properties as those of the unpolarized one, where the atoms become impenetrable and behave as they were noninteracting and spinless.

DFT provides a method through which we can access larger systems beyond the reach of QMC and DMRG simulations.
In the following we study the polarized system confined in a trap with particle number of $N_f=40$,
which is not accessible by means of the present exact diagonalization method. Contour plots are shown in Figs. \ref{fig:eight} and \ref{fig:nine}, respectively, for $p=0.1$ and $0.7$. A clear signature of $2k_{\rm F}\rightarrow 4k_{\rm F}$ crossover is signaled by the emergence of $N_f$ peaks at the
strong interaction strength.

From the above discussion, we find that, in spite of the short-range nature of the interaction, density profile shows pronounced well-separated $N_f$ peaks at strong repulsive interactions.
However, the densities between the peaks do not drop to zero, which is different from the 1D system of long-range Coulomb interaction, where they drop almost to zero in some sense resembling a charge density wave and a quasi-Wigner molecule.

\section{Conclusions}
In this work, we study a 1D system of two-component Fermi gases with a contact repulsive interaction.
The unpolarized or polarized atoms are either confined in a 1D box or subjected to a strongly anisotropic harmonic potential.
The total and spin-resolved densities are calculated within the Bethe-ansatz based spin-density functional theory.
The results are compared to those from the exact Bethe-ansatz method and the exact diagonalization scheme. We found that the Bethe-ansatz based SDFT gives a faithful description for the ground state properties at weak interaction strength but exaggerates the amplitude of the density distributions especially for the corresponding spin-up and spin-down densities at strong interaction strength. In spite of the short-range nature of the interaction, a pronounced $N_f$-peak structure is observed in the density profile in the strongly interacting regime.

For unpolarized systems, the density is characterized by $2k_F$-Friedel oscillations with $N_f/2$ peaks at the weak interaction regime.
As the interaction strength increases, the number of peaks in the density profile is doubled.
This leads to the emergence of $4k_F$-Wigner oscillations of $N_f$ peaks in the density profile. Numerically we found a threshold interaction strength $\lambda_c$ at which the $2k_F\rightarrow 4k_F$ transformation happens. For polarized systems, at weak interaction strength, the peaks in the density profile depend on the system parameters. However, when increasing the interaction strength,
a threshold value can be found where $N_f$-peak oscillations appear in the density profile signaling the $4k_F$-Wigner oscillations.
At strongly repulsive limit, the total energy and the total density profile of the system own the same properties, as those of
the fully unpolarized one. There, the atoms become impenetrable and behave as they were noninteracting and spinless.

{\it Acknowledgments}
This work was supported by NSF of China under grant nos. 11174253 and 10974181, Zhejiang Provincial Natural Science Foundation
under grant no R6110175. It is a pleasure to thank Giovanni Vignale, Marco Polini, Shu Chen, and Wei Li for several useful discussions.

redpajama_set_name: RedPajamaArXiv


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Comparable training and/or experience can be substituted for degrees when appropriate.
Our team is made up of a dedicated group of researchers, scientists, communicators, campaigners, and advocates from wide-ranging backgrounds and experiences. We are committed to building a diverse and inclusive team and a collaborative and supportive work environment where all staff can thrive. We continually strive to create an environment which is a welcoming place for the LGBTQ+ community, people of color, parents, empty-nesters, and people with a wide variety of interests and backgrounds.
During the coronavirus pandemic our staff are working from home. We will resume working from our offices, travel, and in-person meetings when it is safe to do so.
To Apply: We know there are great candidates who won't check all of these boxes, and we also know you might bring important skills that we haven't considered. If that's you, don't hesitate to apply and tell us about yourself. Please upload a cover letter and resume. In the cover letter, please confirm that the listed salary meets your expectations. Upload materials in Word or PDF format only. No phone calls, please.


Interview: If Orlando wasn't terorrism, why do gays feel terrorized?
Greggor Mattson, interviewing Lisa Stampnitzky, author of Disciplining Terror: How Experts Invented "Terrorism" and Politics Lecturer at Sheffield University. GM: Experts have been walking back classifications of Omar Mateen's massacre at Orlando's pulse nightclub as terrorism. And yet, LGBTQ people have consistently described the attack as terrorism. How can we understand the different understandings of … More Interview: If Orlando wasn't terorrism, why do gays feel terrorized?
Leave a comment Interview: If Orlando wasn't terorrism, why do gays feel terrorized?


Programme - 60 Minutes Of Classical Music.
Learn how to play the trombone and how to read music!
Drinks, Music & Cheese & Biscuits!
Tickets are also available online, please click the button below to head to our online ticketing page.
It promises to be a great night and we cannot wait to see you there!
An outstanding night of Opera, starring some very special guests. Whether you're a lover of Opera already or have never attended a performance in your life, this is a night not to be missed!


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A Family Affair: Hope MacVane and The Cliff Island Store & Café
For Hope MacVane, Cliff Island is a family affair – she grew up there, her children have spent summers there, and now she manages the Cliff Island Store just like her parents did in the 80s.
Hope said she gets to see some amazing sunrises and sunsets from the Cliff Island Store & Cafe – how could you not love a place like that?
The Cliff Island Store & Café has been a mainstay on the island for generations, and Hope has been there through a few of its many transformations – first working at the store when she was a Portland High School student and, later, managing the store after she graduated college. This spring when she heard the owners were looking for someone to run the store, the South Portland High school teacher figured if she was going to be working hard during her summer break, she might as well be doing it in a place she loves.
Each year around Memorial Day, the store opens its doors for visitors from all around the world. This year, throughout the summer, Hope has worked to add some specialty items like Union Co. Bagels, Botto's Breads, Coffee by Design, local beers and lobsters, Standard Baking goodies, and fresh veggies from Cultivating Communities to the store's stock of essentials. She said this process has been a little bit of trial and error
Hope MacVane worked at the Cliff Island Store & Cafe in high school, and just wrapped up a summer as manager.
throughout the summer, but she loves seeing the look on a customer's face when she gets something in that they've requested.
When we asked what keeps drawing her back to the island, she said emphatically "the people really make this place the best." Cliff Island has the smallest year-round population of the islands we serve, and, according to Hope, that means people look out for each other.
For some of our lucky deckhands, that means a special treat at the end of a run.
When you walk into the Cliff Island Store & Café, you'll spot some names up on the "Ice Cream Fairy Board" meaning someone has treated them to an ice cream cone. Hope says that several of our deckhands have found themselves on the board as a thank you for a job well done.
We see what Hope means, there's something about Cliff Island.
Hope had us blushing when she said how much she appreciates our hardworking captains, deck hands, and freight crew. "We wouldn't be here without Casco Bay Lines," she said. "How am I going to get ice cream, produce and bread without them? They get us what we need and are so supportive."
With summer winding down, Hope and her family have begun to think again about school bells and classrooms. Life on Cliff Island will return to its regular (peaceful) pace and the store will shut down for the season. For now, you can still grab an ice cream cone on the weekend or pick up some provisions off the noon and afternoon boats during the week. Hope says they'll run that schedule for a few weeks and re-evaluate their official closing date in mid-September.
We've said it before and we'll say it again – there's something truly magical about these islands that keeps us all coming back for more. The spirit of community and tradition is like no other. And Hope's family tradition of caring for her community on Cliff Island is a great example.
We really love delving a little deeper into what makes each island unique and love when you join in! We've received a ton of great photos as part of our #CruiseCascoBay photo contest, so keep 'em coming –we'll be drawing a winner every week through September 14.
From time to time on our blog we'll be featuring stories from island residents. Casco Bay Lines remains committed to fostering strong relationships with our island communities. If you have an interesting story, feel free to reach out to us.
Tags: Island Community
Meet the Crew: An Overdue, Socially Distant Introduction to our New Port Engineer
Philip Lee: An Artist's Eye for Detail
Making Summer Memories with your Little Explorers
Cheers (and Beers) for Casco Bay's Fort Gorges!
Don't Own a Boat? No Problem!


Headlines in Russian cut and contain error special characters such as н &#1090 and others. It started about a week ago. Tested on Windows 7 (Russian regional settings) in FireFox 34 and IE 11 in http://www.gazeta.ru/export/rss/first.xml http://www.i-mash.ru/news/rss.xml and others.
Switch to Russian language interface does not solve the problem. Attaching a screenshot.
Ever since the last update many if not all my rss feeds aren't working correctly. Before the update there weren't any issues with any of the feeds. Just about every day some feeds don't show the latest articles while other do, and if I go directly to the RSS feed page it does show the latest. Also feeds I have marked as read show up as unread so I end up with 3 to 15 unread when all but 1 if any have already been marked as read.
Reader view is not showing all feeds for older items, since the latest update. Only some, random, feeds are showing older items. If I look at individual tabs, I see more items for that tab. Having to look at tabs individually kind of misses the point, yes?
so it can be used in Learning Management Systems.
I would like the ability to sort my feeds in ascending date order (so I read the oldest first). Thank you.
For the last few days, I've been unable to open links when I click on ANY of the "widgets" on my Dashboard.
For example, I have a simple widget that lets me lauch a new tab in Google Bookmarks. However, when I hover my mouse over the widget I now get a "cross hair" cursor (rather than the usual cursor you get when you hover over a link), and nothing happens.
This is making NetVibes virtually useless for me.
Netvibes keeps marking (from my point of view quite randomly) old read items as unread and showing them to me again and again, day after day. This makes the reader quite frustrating to use, even perhaps quite unpractical.
My Twitter widget won't refresh unless I do it manually. That's enough for me to find an alternative to Netvibes if it isn't fixed soon.
I cannot access my bloglines page and I always used to be able to. What has gone wrong.
Can anyone help. I can no longer access my Bloglines page. Please help me.


Alphachain Capital, an FX and cryptocurrency prop trading firm, is seeking to hire a number of new and experienced prop traders to join our trading floor and manage our capital. Those who are successful will begin trading as a full-time independent Junior Prop Trader across major FX markets with a guaranteed $10k trading account. Capital increases will be provided at set target achievements.
Alphachain Capital is a leading proprietary cryptocurrency & FX trading firm based in London and Surrey. The firm specialises in short-medium term positions in large-cap cryptocurrencies and major FX markets and is now seeking to bring on a number of talented individuals who have the motivation and passion to become professional traders.
We are seeking both experienced and new prop traders to join our trading floor and manage our capital. Our trading team includes experienced traders with extensive institutional experience at top tier banking institutions who manage the company's capital and help to train our juniors traders.
Successful candidates will have a passion for the industry and motivated to learn to trade professionally at one of the UK's leading FX & cryptocurrency trading firms.
Those who are successful will begin trading as a full-time independent Junior Prop Trader across major FX markets with a guaranteed $10k trading account. Capital increases will be provided at set target achievements.
If you do not have a 12-month profitable track record and pass the initial interview stages you will be required to attend our 4-week CPD certified Junior Trader Programme. It is an intensive CPD certified training programme for those serious about a trading career in financial markets, delivered by experienced traders and mentors.
There is a fee payable for students attending the training due to trader mentoring, platform implementation costs and allocation of a seat on our trading floor.
Those who pass the interview process will be invited to join the Junior Trader programme with guaranteed starting capital $10,000 to trade their own book as a Junior Trader.
Those with at least a 12-month profitable track record can join our Trader Incubator programme with the potential of immediate funding.
Limited positions available so please apply promptly.
The role is based on our trading floor is based in Redhill, Surrey (30 mins from London Bridge or Victoria).
First year OTE of £50,000, remuneration based on performance. Since proprietary trading is 100% performance based, this is a commission-based role.
All applicants will be automatically subscribed to our mailing list. If you would like to be excluded please let us know at application.


Here at loveit coverit we know that being without your phone can be difficult enough without battling against lengthy and complicated online claim forms.
Our claim process has you, the customer, at its heart. We make things easy and straightforward so you can be reunited with your device as quickly as possible.
Claim hotline number 01702 568081 – our loveit coverit team are waiting to help you Monday to Friday 9am to 5.30pm.
Advise the police within 48 hours if there has been loss or theft of your device and obtain a crime reference number. You must also inform your network provider within 24 hours of discovery of loss or theft so that they can place a block on your device.
Advise us by telephone as soon as possible on the claims hotline number 01702 568081 or via email, support@loveitcoverit.com and we will then provide you with a password protected link to our claim form portal.
Provide at your own expense a fully completed claim form and all details and evidence as may be reasonably required within 30 days of receipt from the incident date. We will not proceed with your claim until all required information has been supplied but once we have all the required claim form and supporting documentation we will confirm our decision on your claim and guide you through our repair or replacement process. Where you are making a claim for accidental damage, liquid damage or mechanical breakdown you may be asked to send your device to us. You will be responsible for the cost of posting your device to us.
In the event of a claim you must be able to provide proof of usage from your network provider that confirms your device has been in use since policy inception and up to the event giving rise to your claim.
Proof of purchase – this should show both the IMEI of the device purchased along with the date/time as well as the store it was purchased from.
Pin number – our engineers will require this to complete quality assurance testing once the repairs have been completed.
Step 1. Go to "Find My iPhone" on iCloud.com.
Step 2. Click "all devices". Select the device.
Step 3. When the device is erased, click "Remove from Account".
Proof of SIM card replacement – when you order a replacement SIM card the document from your Network provider would be sufficient.
Step 1. Go to "Settings" > "Accounts". Select "Google" and select the account you want.
Step 2. Tap the menu icon. Select "Remove account".
Step 3. Click "Remove account" on the pop up and confirm to delete your Google account from Android.
Note – removing the account will delete all of its messages, contacts and other data from the device.
Your username is the email you used when you initially set up your policy.


27:1In the beginning of the reign of Jehoiakim the son of Josiah, king of Judah, came this word unto Jeremiah from Jehovah, saying, 27:2Thus saith Jehovah to me: Make thee bonds and bars, and put them upon thy neck; 27:3and send them to the king of Edom, and to the king of Moab, and to the king of the children of Ammon, and to the king of Tyre, and to the king of Sidon, by the hand of the messengers that come to Jerusalem unto Zedekiah king of Judah; 27:4and give them a charge unto their masters, saying, Thus saith Jehovah of hosts, the God of Israel, Thus shall ye say unto your masters: 27:5I have made the earth, the men and the beasts that are upon the face of the earth, by my great power and by my outstretched arm; and I give it unto whom it seemeth right unto me. 27:6And now have I given all these lands into the hand of Nebuchadnezzar the king of Babylon, my servant; and the beasts of the field also have I given him to serve him. 27:7And all the nations shall serve him, and his son, and his son's son, until the time of his own land come: and then many nations and great kings shall make him their bondman. 27:8And it shall come to pass, that the nation and the kingdom which will not serve the same Nebuchadnezzar king of Babylon, and that will not put their neck under the yoke of the king of Babylon, that nation will I punish, saith Jehovah, with the sword, and with the famine, and with the pestilence, until I have consumed them by his hand. 27:9But as for you, hearken ye not to your prophets, nor to your diviners, nor to your dreams, nor to your soothsayers, nor to your sorcerers, that speak unto you, saying, Ye shall not serve the king of Babylon: 27:10for they prophesy a lie unto you, to remove you far from your land, and that I should drive you out, and ye should perish. 27:11But the nation that shall bring their neck under the yoke of the king of Babylon, and serve him, that nation will I let remain in their own land, saith Jehovah; and they shall till it, and dwell therein. 27:12And I spake to Zedekiah king of Judah according to all these words, saying, Bring your necks under the yoke of the king of Babylon, and serve him and his people, and live. 27:13Why will ye die, thou and thy people, by the sword, by the famine, and by the pestilence, as Jehovah hath spoken concerning the nation that will not serve the king of Babylon?27:14And hearken not unto the words of the prophets that speak unto you, saying, Ye shall not serve the king of Babylon; for they prophesy a lie unto you. 27:15For I have not sent them, saith Jehovah, but they prophesy falsely in my name; that I may drive you out, and that ye may perish, ye, and the prophets that prophesy unto you. 27:16Also I spake to the priests and to all this people, saying, Thus saith Jehovah: Hearken not to the words of your prophets that prophesy unto you, saying, Behold, the vessels of Jehovah's house shall now shortly be brought again from Babylon; for they prophesy a lie unto you. 27:17Hearken not unto them; serve the king of Babylon, and live: wherefore should this city become a desolation?27:18But if they be prophets, and if the word of Jehovah be with them, let them now make intercession to Jehovah of hosts, that the vessels which are left in the house of Jehovah, and in the house of the king of Judah, and at Jerusalem, go not to Babylon. 27:19For thus saith Jehovah of hosts concerning the pillars, and concerning the sea, and concerning the bases, and concerning the residue of the vessels that are left in this city, 27:20which Nebuchadnezzar king of Babylon took not, when he carried away captive Jeconiah the son of Jehoiakim, king of Judah, from Jerusalem to Babylon, and all the nobles of Judah and Jerusalem; 27:21yea, thus saith Jehovah of hosts, the God of Israel, concerning the vessels that are left in the house of Jehovah, and in the house of the king of Judah, and at Jerusalem:27:22They shall be carried to Babylon, and there shall they be, until the day that I visit them, saith Jehovah; then will I bring them up, and restore them to this place.


text:
Lynn Cahoon
New York Times & USA Today Best Selling Author
MEET LYNN
Picture Perfect Frame
Tourist Trap Series, Book 12
In the newest Tourist Trap mystery from the New York Times and USA Today bestselling author, a new art studio has opened in the coastal California town of South Cove—but it's about to turn into a crime scene . . .
As the owner of Coffee, Books, and More, Jill Gardner likes to support other Main Street businesses, so she attends a paint-and-sip event where, sadly, her brushstrokes look more like blobs. It's still fun, though—aside from some disruption by a couple doing more sipping than painting. Jill's police-detective boyfriend is on alert, but a designated driver volunteers to take the drunken pair back to their bed and breakfast, and everything seems resolved. Until the wife's body turns up the next morning back in the studio.
The victim, Nan, is from out of town, so it's hard to imagine who'd have a motive aside from her spouse. Now, in between puzzling over her fortuneteller neighbor's strange behavior, preparing for her best friend's wedding, and pouring cups of java at the bookstore, Jill must uncover the secrets of Nan's life and find out who wanted her out of the picture . . .
NY Times Best Selling Author
© 2022 by Lynn Cahoon


The retired Space Shuttle program and the International Space Station represent the funds expended on human spaceflight over the last 40 years,whichis equivalent to the funds and the time necessary to send humans to Mars. Some would argue that the funds and time expended could have meantmultiple human cheap air force ones missions to Mars and maybe even a permanent presence. But the American human spaceflight program chose a less costly path, one more achievable staying close to home..
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Charlie found us
The shelter named him Coco. No, not THAT Coco but a little boy Coco. He was a mess. Found on the street, he was so matted you could barely see his eyes. The hair was so tightly stuck to his skin it must have been painful. He was stinky, didn't have all his vaccinations, and was the friendliest dog you ever met. He didn't need just a bath or grooming. He needed a total shave. He also needed to have his teeth checked and be neutered and have blood work and all sorts of other diagnostic tests done. His tail never stopped wagging. As much as he could walk because the hair on his body was so stuck, he had a pep in his step. He tried to trot. He smelled awful and was sticky. He made very distinct eye contact and looked just so sad. Finally he walked through the doggy door back into his kennel and just lay down, facing his potential adopter. He had been so neglected for so long no one really knew what kind of dog he was. But the guess was a Shih Tzu, Havanese, Lhasa Apso or all three!
After several hours spent looking at each other, and then taking slow steps for a short walk, a love match was made. The volunteers kept coming by asking if he was going to be adopted. His potential adopter was hooked.
But a serious plan had to be devised. He couldn't go straight home where there were other dogs because he was not fully vaccinated and no fecal had been done. What if he had parasites or worse? It was not safe to bring him home. So plans were made to bring him directly to his new mom's vet and they would do everything that needed to be done to bring out the beauty that was already in his spirit. The list is long: total shave, blood work, dental exam, complete his vaccinations, fecal test, heart exam, neuter and who knows what else. But he was in excellent hands now and step by step he would be cared for and his health determined. So he was adopted and pranced out to freedom.
He will be at the vet for a while getting everything done and his health status assessed, Once he is stable he will meet his new brother and sister who will be brought to the clinic to meet him in a neutral spot.
Coco is now Charlie and all mine!
Free Orientation
Our last class visit
Benny was asked to do an interview for a Channel 8 Las Vegas Now segment discussing our volunteer work with Southwest Medical Hospice and he aced it! He is a true Hospice Hero and I am proud to be at


The top-of-the-line short cuffed racing glove from Garibaldi, the Carbotech, boasts numerous features and is leader in its category. It combines holed Goat Nappa on back and top quality Goat DD leather on palm for an utter suppleness. Pre-curved finger construction for a better fit and feel. Bmb fit wrinkle-free inner lining for a maximum comfort and grip. Varnished carbon protector on knuckles with hi-visibility TPR. Exclusive TPR protector on lower back. TPR thermoplastic polyurethane resin protectors on fingers. Microfiber reinforcement on little finger with soft EVA padding. Leather reinforcement on thumb and palm with EVA padding and TPR. Leather and elastic fabric fourchette inserts between fingers for a better dexterity and elasticated accordion leather inserts on fingers for a better flexibility. Microfiber reinforcement on palm with silicone artwork. Stretch on cuff. Wrist adjustment for a customized and tight fit. Reflective. CE 13594:2015 homologation. Black colour coming in next November 2018.


When Should We Stop Prescribing?
Hormonal Therapy for Early Breast Cancer: Do We Learn From Past Mistakes?
The U.S. Food and Drug Administration (FDA) approved bevacizumab (Avastin) in combination with paclitaxel, pegylated liposomal doxorubicin, or topotecan for the treatment of patients with platinum-resistant, recurrent epithelial ovarian, fallopian tube, or primary peritoneal cancer.
Childhood Obesity and Leukemia: Is It Time to Intervene?
Sigmoidoscopy or Colonoscopy for Colorectal Cancer Screening: Is It Still the Question?
With approximately 22,000 diagnoses annually in the United States, ovarian cancer isn't among the most commonly occurring cancers. Yet, the mortality rate for women who have ovarian cancer hovers above 60%.
Now in Spanish on Cancer.Net: Managing Your Weight After a Cancer Diagnosis, and More!
In 6 out of 10 cases, ovarian cancer is diagnosed when the disease is advanced and 5-year survival is only 27%. A new study suggests that a cancer-killing virus combined with a chemotherapy drug might safely and effectively treat advanced or recurrent forms of the disease.
The following seven recipients of the 2014 Conquer Cancer Foundation of ASCO Merit Awards in Palliative Care were honored at the 2014 Palliative Care in Oncology Symposium for their work in improving the care of people living with cancer around the world.
The American Society of Hematology (ASH) recently announced the election of four new members to its Executive Committee, the governing body of the organization, for terms beginning after the 2014 ASH Annual Meeting, which will be held December 6–9 in San Francisco.
A collaborative team of leaders in the field of cancer immunology from Memorial Sloan Kettering Cancer Center has made a key discovery that advances the understanding of why some patients respond to the CTLA-4 blocking antibody ipilimumab (Yervoy), an immunotherapy drug, while others do not.
The following essay by Carolyn D. Runowicz, MD, is adapted from The Big Casino: America's Best Cancer Doctors Share Their Most Powerful Stories, which was coedited by Stan Winokur, MD, and Vincent Coppola and published in May 2014. The book is available on Amazon.com and thebigcasino.org.
Fred Hutchinson Cancer Research Center announced that it has named D. Gary Gilliland, MD, PhD, an expert in cancer genetics and precision medicine as its new President and Director. He will take the helm as the Center's new leader on January 2.
The National Comprehensive Cancer Network (NCCN) has published the 20th annual edition of the NCCN Clinical Practice Guidelines in Oncology (NCCN Guidelines) for Non-Small Cell Lung Cancer (NSCLC), one of the eight original NCCN Guidelines published in November 1996.
PRC2 (polycomb repressive complex 2) has been shown to promote oncogenesis in many tumor types; however, loss of function mutations in PRC2 components has also been shown to occur in some hematopoietic malignancies, raising questions about the precise role of the complex in cancer.
In a study reported in Journal of the National Cancer Institute, Wang and colleagues found that adding an mTOR inhibitor to cetuximab (Erbitux) resulted in marked improvement in antitumor activity in squamous cell carcinomas of the head and neck expressing PIK3CA and RAS oncogenes.
I read with great interest your interview with Virginia LeBaron, PhD, APRN, about barriers to adequate pain control ("Despite Growing Awareness, the Global Crisis of Untreated Cancer Pain Persists," The ASCO Post, October 15, 2014).


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