VIMS Data Management App(Door-to- Door) is one the best election campaign management applications, available. Especially hand tailored for the client, VIMS Data Management App(Door-to- Door) gives access to all the relevant data of the assembly/parliamentary in easy to understand statistical forms, Leadtech Voter Information Management System VIMS Political Door To Door Survey App.
The entire door to door survey process can be categorized into three steps.
Caste equations: Research to collect the caste statistics in the assigned assembly/parliamentary. These statistics help the political leader to identify their vote share in the area.
A team of surveyors/investigators under the supervision of a project manager initiate the exhaustive survey process to visit every household in the assigned assembly/parliamentary. This is done by a visit to every house on the voters' list of the assembly/parliamentary. This process though variable takes on an average of 45-60 days. The collected data is the then organized and sent for the technical team for verification and analysis.
The statisticians further organize the collected data and prepare the statistics for analysis. These statistics are then analyzed and a final report is prepared for the client. The final reports consist of graphs and comments/advice of statisticians on the same.
Right after step 1 'The Questionnaire Creation' the questions are fed to the VIMS Data Collection App(Door-to- Door), making all the questions accessible to the surveyors/investigators spread across the assembly on their android mobile phones/tablets.
Voter list Search: To ensure the accuracy of the each responder's data is mapped to their voter id. They can search and filter the list by their Name, House Number or Father's/Mother's name.
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The VIMS Data Management App(Door-to- Door) is one the best election campaign management applications, available. Especially hand tailored for the client, VIMS Data Management App(Door-to- Door) gives access to all the relevant data of the assembly/parliamentary in easy to understandstatistical forms.


Contact Dr. Crivelli at drcrivelli@yahoo.com to attend hands-on sessions.
Doctors and CA trainees, please note. You do NOT need to finish the video portion of the course to attend hands on sessions. In order to complete the requirements by the deadlines, start attending them as soon as possible.
Important Notice: CAs are required to be registered as a "CA Applicant" as soon as they are hired. There are stiff penalties if a CA is found working without first being registered with the board so please do not delay registering any new CAs. CA applicants must complete all requirements within 11 months of registration so their application and documentation can be submitted and they can complete their examination within a one-year period of hire. Dates of examination can be found in the "Upcoming Events" section of the Board of Examiners Website (link to http://www.mdchiro.org/) . CAs must complete their online and hands on training, show a certificate of "Provider Level" Red Cross or American Heart Association CPR training, and submit them with documentation of 480 hours in office training 30 days prior to the date of examination. It is the Supervising chiropractor's duty to document 480 hours of in service training. They are also required to complete 3-hours of Jurisprudence and Risk Management training however those hours will be provided by the Board on the day of the examination. Any questions regarding the duties of a supervising chiropractor or the CA application process should be made directly to the Board of Examiners at (410) 767-6500.


text:
National Hockey League 1964/1965 var den 48:e säsongen av NHL. De 6-lagen spelade 70 matcher i grundserien innan Stanley Cup inleddes den 1 april 1965. Stanley Cup vanns av Montreal Canadiens som tog sin 13:e titel, efter finalseger mot Chicago Black Hawks med 4-3 i matcher.

Ulf Sterner blev denna säsong den andre svenske ishockeyspelare att spela i NHL efter Gus Forslund som spelade i NHL säsongen 1932/1933. Sterner tillhörde New York Rangers och spelade fyra matcher utan att göra någon poäng.

Chicago Black Hawks-spelaren Stan Mikita vann poängligan för andra året i rad. Säsongen 1964/1965 fick han ihop 87 poäng, 28 mål och 59 assist.

Grundserien

Poängligan 1964/1965
Not: SM = Spelade matcher, M = Mål, A = Assists, Pts = Poäng

Slutspelet 1965
4 lag gjorde upp om Stanley Cup-bucklan, matchserierna avgjordes i bäst av sju matcher.

Semifinaler

Detroit Red Wings vs. Chicago Black Hawks

Chicago Black Hawks vann semifinalserien med 4-3 i matcher

Montreal Canadiens vs. Toronto Maple Leafs

Montreal Canadiens vann semifinalserien med 4-2 i matcher

Stanley Cup-final

Montreal Canadiens vs. Chicago Black Hawks

Montreal Canadiens vann finalserien med 4-3 i matcher

NHL awards

All-Star

Källor
 NHL.com - Säsongen 1964/1965

1964 i Kanada
1964 i USA
1965 i Kanada
1965 i USA
Ishockeysäsongen 1964/1965
1964/1965

redpajama_set_name: RedPajamaWikipedia


Open "Just Cause 3" folder, double click on "Setup" and install it.
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I have intel i3 7th generation . Is this game running .


text:
Issues and downloads 2014 August 2014 Don't Get Me Started - Unwritten Rules
Don't Get Me Started : Unwritten Rules
David Platt | August 2014
The software industry, like modern society in general, is guided by many written rules, and it's accumulating more all the time. But the older and wiserless stupid more cynical I get, the more I see that both society and the software industry are actually governed more by unwritten rules rather than written ones.
The written rule says: "Thou shalt not do X!" The unwritten rule says, "Yes, you can do X, at least under certain circumstances. You sort of have to in order to get the job done." The former addresses the world as the writer wishes it were; the latter as it actually is.
Complicated? Sure. Nuanced? Definitely. Trouble? Often. But observe the next time an airline pilots or nurses union stages a work-to-rule job action instead of a strike. Without the lubrication of these unwritten rules, their workplaces quickly grind to a gridlocked halt. And so would society if we didn't follow unwritten rules instead of written ones.
Consider Michael Pineda, the New York Yankees pitcher who In April received a 10-game suspension for using pine tar on his fingers to better grip the ball. The written rule says that pitchers can't use pine tar or any other substance. The unwritten rule says that a little pine tar is OK in cold weather, as long as you're discreet about it. Pineda was suspended not so much for using pine tar, but for doing it so blatantly that the umpires had to take notice (you can read about it at foxs.pt/1i3R3fz).
To take an example from our industry, object-oriented programmers have long declared global variables to be taboo. You should be shot for even thinking about them, right? On the other hand, what's a class static, except for a global dressed up in wrappers to make it politically correct? Programmers often hang them from an object class named "Globals." When there's only one instance of something in a program, and it's an integer, how many layers of abstraction and managers and services do you want me to wrap it up in to allow you to feel virtuous? As your blood pressure skyrockets from reading that last sentence, I'll rephrase the question: How many layers are you willing to pay me for, when you could use that money for something else? Your check is your answer. And it's probably different from your first reaction two sentences ago.
Sometimes the written rule consists solely of writing down the pre-existing unwritten rule. Hardwiring a string, such as a file name, directly into your code is usually a bad idea; but sometimes you have to do it. Give that construction a virtuous-sounding label and now you're being good.
"We're following the 'Well Known Name' design pattern," says the geek. "Good, good," says the non-technical boss. "I'm glad you're using design patterns instead of that cowboy coding thing I've heard about."
Guys, you're hardwiring in a string. Do that when you need to, with your eyes wide open, when you've thought it out carefully and know that the benefits outweigh the costs. Soothe your uneasy feelings with the lie that you'll come back and fix it someday when you get the time. But don't think you're changing what it does by dressing up its name. A bug hurts and angers your user no less when you call it an issue (see msdn.microsoft.com/magazine/ff955613).
Charting a course through these minefields, knowing when to follow the written rules and when to ignore them in favor of the unwritten ones, is what software engineering is about. There are few, absolute, "thou shalt not" rules in this business (although not scrolling a marquee string in your browser's status bar comes darn close). The one thing I always tell my clients and students is, "Thou shalt think. If that's hard, then thou shalt pay me to help you think."
I'm curious to hear your favorite unwritten rules of software development—or anything else, for that matter. Send them to me at dave@rollthunder.com.
I'm sure that some pedantic geek will now say that because I've written some rules here, they aren't unwritten any more. To which I reply: You're breaking my unwritten rule against nit-picking your hyperbolic back-page columnist. That's worth a 10-game suspension, don't you think?
David S. Platt teaches programming .NET at Harvard University Extension School and at companies all over the world. He's the author of 11 programming books, including "Why Software Sucks" (Addison-Wesley Professional, 2006) and "Introducing Microsoft .NET" (Microsoft Press, 2002). Microsoft named him a Software Legend in 2002. He wonders whether he should tape down two of his daughter's fingers so she learns how to count in octal. You can contact him at rollthunder.com.

redpajama_set_name: RedPajamaCommonCrawl


text:
Q: How can I pass my get request into my res.render? const router = require('express').Router();
const request = require('request');

router.get('/', (req, res) => {

    request({
        url: 'https://discordapp.com/api/users/@me/guilds',
        auth: {
            'bearer': req.user.accessToken
        }
    }, function (err, res) {
        console.log(res.body);
        //How can I pass the res.body from here
    });

    res.render('dashboard', {user: req.user servers: /*into here?*/});
});

module.exports = router;

How can I pass my get request into my res.render? So I can output it using ejs.

A: res.render should be called in a place where necessary data is available.  If this place is request callback then that's it. Since there are different res objects in different function scopes, then need to be named to not be shadowed:
request({
    url: 'https://discordapp.com/api/users/@me/guilds',
    auth: {
        'bearer': req.user.accessToken
    }
}, function (err, response) {
   res.render('dashboard', {user: req.user, servers: response.body});
});

redpajama_set_name: RedPajamaStackExchange


text:
\section{Result}
\subsection{Concept of the plasma-assisted laser spectroscopy}
In the present experiment, we prepare the (4$d^{9}_{5/2}$5$s$)$_{J=3}$ metastable state of $^{127}$I$^{7+}$ in an EBIT and irradiate a pulse laser to the trapped HCI, as shown in \textbf{Fig.~1~a}.
\textbf{Figure~1~b} shows the experimental scheme used here with the level structure of $^{127}$I$^{7+}$.
Due to the closed 4$d^{10}$ shell structure in the ground state, the excitation energy to the first excited fine-structure level (4$d^{9}_{5/2}$5$s$)$_{J=3}$ is relatively high at approximately 47 eV.
Although such high-energy states are generally de-excited in a short time, the lifetimes for every hyperfine-structure level in (4$d^{9}_{5/2}$5$s$)$_{J=3}$ are longer than 10~s because their de-excitation processes are strongly forbidden, except for $M3$ and hyperfine-mixing $E2$ transitions.
From the long-lived fine-structure level, the extreme ultraviolet (EUV) electric-quadrupole ($E2$) transition ((4$d^{9}_{3/2}$5$s$)$_{J=2}$ $\rightarrow$ (4$d^{10}$)$_{J=0}$)  was induced by pulsed laser excitation $via$ the $M1$ transition ((4$d^{9}_{5/2}$5$s$)$_{J=3}$ $\rightarrow$ (4$d^{9}_{3/2}$5$s$)$_{J=2}$).
Both the initial and excited levels in the laser excitation are metastable states without any $E1$ decay path; thus, the natural width of the transitions is estimated to be $\sim$10$^{-5}$ cm$^{-1}$ from the theoretical 4 $\mu$s lifetime of the upper fine-structure level (4$d^{9}_{3/2}$5$s$)$_{J=2}$.
The intrinsically narrow natural width of the laser transitions contributes to the high-resolution in spectroscopic measurements, revealing the hyperfine-structure.

\begin{figure}[t]
\includegraphics[width=8.5cm]{New_Fig1_ver7.pdf}
\caption{\label{Concept} \textbf{Schematic diagram of the present laser spectroscopy.} \textbf{a.} Brief overview of the experiment. \textbf{b.} Experimental scheme with the energy diagram of $^{127}$I$^{7+}$. The population rate to (4$d^{9}_{5/2}$5$s$)$_{J=3}$ was estimated, using collisional-radiative modeling \cite{Kimura2020}. An electron energy of 105 eV and a density of 10$^{10}$ cm$^{-3}$ are assumed in the collisional-radiative rates, corresponding to the present experimental condition. The energy structure and lifetime were calculated using GRASP2018 \cite{GRASP}.}
\end{figure}

\begin{figure*}[t]
\includegraphics[width=17.4cm]{New_Fig2_ver3.pdf}
\caption{\label{EUVSpectrum} \textbf{Theoretical predictions for the hyperfine-structure splitting in the laser excitation.} \textbf{a.} Statistical weights of the initial state (4$d^{9}_{5/2}$5$s$)$_{J=3}$. \textbf{b.} Spectral intensity ($gA$). \textbf{c.} Zeeman splitting. Solid and dotted lines show the $\Delta m_F = 0$ and $\Delta m_F = \pm 1$ transitions, respectively. \textbf{d.} Doppler broadening simulation. The transition energy was taken from the NIST database \cite{NIST}.}
\end{figure*}

The long-lived state (4$d^{9}_{5/2}$5$s$)$_{J=3}$ of $^{127}$I$^{7+}$ was continuously prepared through collisional and radiative processes in the EBIT plasma.
Although increasing the number of trapped ions necessitates an enhanced electron density of the plasma, electron collisions must be suppressed to detect LIF emissions from the laser-excited fine-structure level with a lifetime in the order of microseconds.
We controllably maintained the EBIT electron density below 10$^{10}$ cm$^{-1}$, where the electron collision rate was apporoximately 10$^3$ s$^{-1}$.
The production rate of (4$d^{9}_{5/2}$5$s$)$_{J=3}$ under an electron density of 10$^{10}$ cm$^{-1}$ was estimated to be $\sim$160 s$^{-1}$ from collisional-radiative modeling \cite{Kimura2020}.
Thus, the excitation rate by the pulse laser was operated at less than 1 s$^{-1}$ avoiding the depletion of the population in the initial state (4$d^{9}_{5/2}$5$s$)$_{J=3}$.
This well-designed closed transition cycle, including the plasma processes, maintains the sequential LIF detection, suppressing the unintended population loss for the initial and excited levels in the laser excitation.
We emphasize that the well-defined laboratory plasma and its control with a deep understanding of excitation and de-excitation dynamics through collisional-radiative modeling allow us the LIF detection, even though the ions are in a plasma.

The hyperfine-structure splitting for each fine-structure level is given by the magnetic-dipole hyperfine-structure constant $A_{hfs}$, the electric-quadrupole hyperfine-structure constant $B_{hfs}$, and the quantum numbers $J$, $F$ and $I$.
$A_{hfs}$ and  $B_{hfs}$ are relevant values to the atomic structure and the nuclear moments.
We calculated these constants and the splittings for (4$d^{9}_{5/2}$5$s$)$_{J=3}$ and (4$d^{9}_{3/2}$5$s$)$_{J=2}$ using the atomic calculation code GRASP2018 \cite{GRASP} as shown in \textbf{Fig.~1~b}.
In general, a contracted electron orbital in HCIs enhances the hyperfine-structure splitting.
Additionally, in the present atomic system, the 5$s$ electron orbital in the HCI has a significant overlap with the nucleus, resulting in the large hyperfine-structure splitting.
In fact, our theoretical calculation shows that the $A_{hfs}$ constant for (4$d^{9}_{5/2}$5$s$)$_{J=3}$ in $^{127}$I$^{7+}$ is six times larger than that for 4$d^{9}_{5/2}$ in $^{127}$I$^{8+}$, even though the binding energy is smaller.

\subsection{Prediction of the spectral profile}
The hyperfine-structures split the laser transition into 14 components, considering the selection rules for $M1$ transitions ($\Delta F=\pm 1, 0$).
Spectral simulations were performed to predict the features of the laser excitation spectrum, including hyperfine-structures.
\textbf{Figure~2~a} shows the statistical weight of the initial state with the wavenumber deviation $\Delta k$ corresponding to the difference from the original transition energy without the hyperfine-structures.
\textbf{Figure~2~b} shows the spectral intensity $gA$, which is the sum of Einstein $A$ coefficients of the $\Delta m_F$=0 transitions for every magnetic sub-level.
We also calculated the Zeeman splitting using the intermediate magnetic field treatment, as shown in \textbf{Fig.~2~c}.
Equations and atomic codes are summarized in the Methods section.
According to the simulation, the $M1$ transition lines are distributed over several cm$^{-1}$, and the spectral features under low magnetic field conditions have an asymmetric profile because of their specific quantum numbers and the intrinsic difference in the Racah coefficient between these transitions.
At high magnetic fields above 0.5 T, such as that in a typical EBIT, magnetic sub-level resolved transitions spread over a wide $\Delta k$ range, which hinders the experimental assignment of hyperfine components.
To overcome this difficulty,  we employed the low magnetic field operation (0.03 T) of a compact electron beam ion trap (CoBIT) \cite{Nakamura2008} at the University of Electro-Communications.
Although this magnetic field is not classified as the weak field limit, it is sufficiently low enough to suppress the Zeeman splitting below 0.05 cm$^{-1}$.
This quasi Zeeman-free condition enables us to resolve the hyperfine-structures.

In the present experiment, line broadening is expected, mainly caused by the Doppler effect due to ion motion in the EBIT, since the Zeeman splitting, laser linewidth, and natural width of the transition are all less than 0.05 cm$^{-1}$.
\textbf{Figure~2~d} shows the spectral broadening simulation under the assumption of a Maxwellian distribution for the kinetic energies of the trapped ions in the EBIT \cite{Orts2007}.
In the low-temperature region, the width of each transition line becomes narrow, and the associated features originating from the $F=7/2$ $\rightarrow$ $F^{'}=7/2$ and $F=9/2$ $\rightarrow$ $F^{'}=9/2$ transitions appear around 17631-17632 cm$^{-1}$.
The simulation shows that the ions should be cooled below 20 eV to characterize the hyperfine-structures and determine the spectroscopic parameters.

\subsection{Measurement of the laser-induced fluorescence}
\textbf{Figure~3} shows the LIF detection in the present experimental setup.
From CH$_3$I vapor, $^{127}$I$^{7+}$ ions were produced by an electron beam and stored in an electrostatic trap potential formed by the electron beam and three successive cylindrical drift-tube (DT) electrodes \cite{Kimura2020}.
To excite the $M1$ transitions, we used a wavelength-tunable dye laser (Sirah Cobra-Stretch with the dual 3000 lines/mm grating option, Exciton Rhodamine 6G/ Ethanol dye solution) pumped by the second harmonic of an Nd:YAG nanosecond-pulse laser (Cutting Edge Optics Gigashot, 10 ns) with a 100 Hz repetition rate.
The wavelength of the laser was monitored using a high-precision wavemeter (High Finesse, WS-6-600).
The laser pulse energy was tuned and maintained at approximately 7 mJ/pulse by the combination of a $\lambda$/2 wave plate and polarizer.
The polarization of the laser was perpendicular to the magnetic field so that only the $\Delta m_F$ = 0 transitions were excited.
LIF was monitored with a time-resolving extreme ultraviolet (EUV) spectrometer consisting of an aberration-corrected concave grating (Hitachi 001-0660) and a position-sensitive detector (PSD, Quantar Technology Inc., model 3391)  \cite{Tsuda2017}.
A typical $^{127}$I$^{7+}$ emission spectrum obtained with the EUV spectrometer is shown in \textbf{Fig.~3~b}.
Owing to the large difference in wavelength, the LIF signal can be readily distinguished from the laser-scattering noise.
The prominent line at 49 eV is the targeted $E2$ transition ((4$d^{9}_{3/2}$5$s$)$_{J=2}$ $\rightarrow$ (4$d^{10}$)$_{J=0}$), which was used to detect laser excitation.
To distinguish the LIF signal from the continuous emission excited by collisional and radiative processes in the plasma, the time spectrum of the $E2$ transition was recorded with a Multi-Channel-Scaler (MCS) as shown in \textbf{Fig.~3~c}.
The observed lifetime of the LIF signal was approximately 4 $\mu$s, which agrees with our theoretical calculation.

\begin{figure}[t]
\includegraphics[width=8.7cm]{New_Fig3_ver5.pdf}
\caption{\label{EUVSpectrum} \textbf{Overview of the LIF detection setup.}
\textbf{a.} Schematic of the experimental setup.
\textbf{b.} Typical EUV emission spectrum.
\textbf{c.} Time-resolved signal for the laser-induced $E2$ transition fluorescence.}
\end{figure}

\begin{table*}[t]
\caption{\label{Results} \textbf{Summary of the experimental and theoretical values for (4$d^{9}_{5/2}$5$s$)$_{J=3}$ and (4$d^{9}_{3/2}$5$s$)$_{J=2}$ in $^{127}$I$^{7+}$.} The theoretical results are obtained by Multi-configuration Dirac-Fock calculations combined with the relativistic configuration-interaction (RCI) approach, as described in the Methods section. The RCI corrections of the generalized Breit interaction and the QED effects (self-energy and vacuum polarization) are separately shown.}
\begin{ruledtabular}
\begin{tabular}{cccccc}
 & \multicolumn{1}{c}{Experiment} &\multicolumn{1}{c}{Theory}& \multicolumn{1}{c}{MCDF}&\multicolumn{1}{c}{Breit} &\multicolumn{1}{c}{QED}   \\
\hline
$A_{hfs}$  [GHz]&10.3($\pm$0.3$_{stat}$  $\pm$0.3$_{sys}$)  &10.39($\pm$0.05)& 10.41&  $-$1.7$\times$$10^{-2}$& $+$3.3$\times$$10^{-3}$ \\
$B_{hfs}$  [GHz]& 2.9($\pm$1.8$_{stat}$  $\pm$0.3$_{sys}$) & 2.32($\pm$0.02)& 2.37&  $-$4.3$\times$$10^{-2}$& $+$4.0$\times$$10^{-4}$  \\
$A_{hfs}^{'}$  [GHz]&15.8($\pm$0.3$_{stat}$  $\pm$0.3$_{sys}$) &15.33($\pm$0.03)& 15.45& $-$1.2$\times$$10^{-1}$& $+$7.5$\times$$10^{-3}$   \\
$B_{hfs}^{'}$  [GHz]&1.5($\pm$1.4$_{stat}$  $\pm$0.3$_{sys}$)  &2.02($\pm$0.01)& 2.05&  $-$2.8$\times$$10^{-2}$& $+$3.0$\times$$10^{-4}$   \\
$k_0$  [cm$^{-1}$]&17633.67($\pm$0.02$_{stat}$  $\pm$0.03$_{sys}$) & 17616($\pm$22) & 18016   & $-$418 & $+$18    \\
\end{tabular}
\end{ruledtabular}
\end{table*}

\subsection{LIF spectrum and its analysis}
\textbf{Figure~4} shows the laser wavelength spectrum of the LIF signal.
It took a few hours to accumulate LIF counts at each wavelength.
To compensate for possible fluctuation in the number of stored ions, the LIF counts were normalized by continuous $E2$ counts, which are regarded to be proportional to the ion number.
The vertical axis in \textbf{Fig.~4} represents the ratio of LIF signal counts within 10~$\mu$s after laser irradiation to the total counts, including the continuous emission within the interval of laser irradiation (10 ms).
The background level due to continuous plasma emission in the ratio was directly determined to be 0.001 from the time range ratio \mbox{(10~$\mu$s/10~ms)}.
In a preliminary scan, a broad main structure at 17633 - 17634 cm$^{-1}$ and associated structures at 17634 - 17636 cm$^{-1}$ were observed.
We considered that the associated structures were important for understanding the origin of the spectral features.
Therefore, a finer wavelength scan of this region was performed to obtain higher statistics, as shown in \textbf{Fig.~4}.
In the fine scan, all DT electrodes were set to the ground potential to suppress the Doppler line broadening.
While the axial potential formed by the electron beam still enables the storage of $^{127}$I$^{7+}$ ions, the resulting shallow axial potential allows for evaporative cooling, yielding a reduction in the spectral linewidth \cite{Beiersdorfer1996, Orts2007}.
Comparing results to the spectral simulation, we conclude that the main and associated features are mainly composed of ${\Delta F}$ = -1 and 0 transitions, respectively.

\begin{figure}[t]
\includegraphics[width=8.6cm]{New_Fig4_ver1.pdf}
\caption{\label{LIF spectrum} \textbf{Experimental LIF spectrum.} The fitting result  is shown with separated profiles for every transition. The error bar for each data point represents the statistical error.}
\end{figure}

To determine the hyperfine-structure constants, the observed spectrum was fitted with a model function incorporating all hyperfine-resolved transitions with the same Doppler width $k_D$.
The model function is described in the Methods section.
The center of the transition energy for each line is determined by the original transition energy $k_{0}$ for the fine-structure transition and the hyperfine-structure constants for each of the initial and excited fine-structure levels.
The relative line intensity for each transition was defined by the simulation intensity in \textbf{Fig.~2~b}.
Consequently, the seven parameters $A_{hfs}$, $B_{hfs}$, $A_{hfs}^{'}$, $B_{hfs}^{'}$, $k_0$, $k_D$, and total spectral intensity $I_0$ were determined in the fitting procedure,
where the primed quantities refer to the excited fine-structure level.
Note that theoretically calculated $A$ coefficients were used to determine the simulated intensities.
The intensity model mainly depends on the Racah coefficients whereas the actual intensity is slightly different because of the hyperfine-structure mixing with other fine-structure levels.
We theoretically evaluated the hyperfine-mixing effect on the transition intensities and found that this contribution is less than 0.05 $s^{-1}$ for every $A$ coefficient.
This ambiguity in the model function affects the determination of the experimental values by less than 1$\%$ of the experimental uncertainty and is thus considered not significant.
The statistical population in the intensity model may also be disturbed by the lifetime difference between hyperfine levels \cite{Trabert2007}.
However, in the case of $^{127}$I$^{7+}$, it is not necessary to consider such possibilities because the radiative decay rates are at least $10^3$ times longer than the collisional-radiative rate supplying the population to the metastable fine-structure level;  hence, the populations are not quenched by spontaneous decay to the ground state.
Thus, we consider the intensity model used here to be reasonable for determining the constants.
The fitted profiles for each hyperfine component and their convolution are shown in Fig.~4.
The obtained parameters are listed in \textbf{Table~I} along with the theoretical values calculated by the GRASP code taking the Breit and quantum electrodynamic (QED) effects into account.
The reduced-chi-square in the fitting was 1.1.
From the laser wavelength stability during the measurement, the systematical errors for the hyperfine-structure constants were estimated to be 0.3 GHz.
The systematic error of $k_0$ is 0.03 cm$^{-1}$ taking the absolute accuracy of the wavemeter into account.
The resulting $k_D$ is 0.46 ($\pm$ 0.04) cm$^{-1}$ corresponding to an ion temperature of 15 ($\pm$ 2)  eV under the assumption that Doppler broadening dominates in the spectral line width.
The shallow trapping potential formed by the zero DT voltage and the thin electron density with a low magnetic field enabled the trapped ions to be evaporatively cooled down to the low temperature similar to that found in forced evaporative cooling by turning off the electron beam \cite{Mackel2011}.
The narrow Doppler width realized in the present measurement is essentially important for resolving the hyperfine splitting.

\begin{figure*}[t]
\includegraphics[width=14cm]{New_Fig5_ver4.pdf}
\caption{\label{Z-Dependence} \textbf{Potential of the present laser spectroscopy for studying heavy nuclei.} Atomic number ($Z$) dependence of the theoretical transition energies in Pd-like and Ni-like ions along with the transition energies of the $E1$ transition 5$s$ - 5$p_{1/2}$ in Ag-like ions is shown for comparison. The purple shaded region indicates wavelength ranges where it is generally difficult for lasers to reach ($<$ 200 nm).}
\end{figure*}

Because the nuclear spin and moments of $^{127}$I are well-known \cite{Moment_Table}, the experimentally obtained hyperfine-structure constants are used to validate the theoretical calculation of the electron orbital for each fine-structure level.
Experimental results obtained here show reasonable agreement with theoretical values, considering uncertainties.
The transition energy $k_0$ obtained by the experiment agrees with the theoretical calculation within approximately 0.1 $\%$.
The Breit interaction shifts the transition energy by 2 $\%$, which is important to reproduce the experimental result.
The energy of each fine-structure level has been compiled in the NIST database \cite{NIST} from several experimental results using passive spectroscopy, and the uncertainty was evaluated to be 100 cm$^{-1}$.
In the present study, we clearly demonstrate that our active spectroscopic approach succeeded in directly measuring the transition energy and greatly improving its uncertainty.
This clarified the importance of the relativistic configuration-interaction (RCI) correction for the Breit interaction.

\section{Discussion}
We have demonstrated laser spectroscopy of forbidden transitions between metastable states of HCIs stored in an EBIT by employing Pd-like $^{127}$I$^{7+}$.
The laser excitation spectrum of the HCIs in a quasi Zeeman-free low magnetic field revealed distinct hyperfine-structures, which provided evidence for the enhancement of the hyperfine interaction via a contracted electron cloud with a 5$s$ valence.
The resulting hyperfine-structure constants of highly charged ions with a $well$-$known$ nucleus provide a benchmark for atomic orbital calculations with relativistic many-electron correlations, allowing for discussion of the electron cloud in the vicinity of the nucleus for each fine-structure level.
Even though the transition observed in this study is not a proposed HCI clock candidate, the building of a benchmark to understand hyperfine-structures in many-electron HCIs makes a significant step toward developing such clocks, especially that the most promising current clock candidates with a 5$s$-4$f$ level crossing \cite{Berengut2010, Berengut2011, Berengut2012-1, Dzuba2012, Safronova2014-1, Safronova2014-2, Safronova2014-3, Dzuba2015, Windberger2015,  Dzuba2016, Nandy2016, Kozlov2018} are intrinsically accompanied by a similar characteristic electron configuration having a single 5$s$ electron.
The established benchmarks would serve as reference to enhance the understanding of the hyperfine interaction in many-electron HCIs.

The present hyperfine-structure-resolved laser spectroscopy offers future possibilities for experimental studies in nuclear physics using HCIs, such as a broad investigation of $unknown$ nuclear spins and moments and hyperfine anomalies with a specialized EBIT for highly charged radionuclide ions \cite{Vondrasek2016}.
Recently, high-precision atomic orbital calculations have been extensively developed to investigate nuclear properties from hyperfine-structure constants \cite{Campbell2011, Safronova2013, Thielking2018, Li2021, Porsev2021}.
While this approach had the privilege for particular nuclei with optically accessible transitions at low valence ions, the extension of the target to HCIs enables the selection of an atomic-level structure by changing the charge state.
In addition, an $ns$-valence state enhancing its hyperfine interaction can be arbitrarily selected, in contrast to neutral atoms or single charged ions whose electron configurations are fixed.
We consider that the present LIF scheme has the potential to be a versatile method for investigating heavy nuclear properties because it can be directly applied to the three transitions in Pd-like ions and Ni-like ions, as follows.
Pd-like ions have an additional excitation pathway from the long-lived (4$d^{9}_{5/2}$5$s$)$_{J=3}$ state to the (4$d^{9}_{5/2}$5$s$)$_{J=2}$ excited fine-structure level via an $M1$-allowed transition.
Ni-like ions have a similar energy level system with the 3$d^{10}$ closed ground state.
Therefore, the investigation of the (3$d^{9}_{5/2}$4$s$)$_{J=3}$ $\rightarrow$ (3$d^{9}_{3/2}$4$s$)$_{J=2}$ and (3$d^{9}_{5/2}$4$s$)$_{J=3}$ $\rightarrow$ (3$d^{9}_{5/2}$4$s$)$_{J=2}$ transitions with the present laser spectroscopy scheme is also possible.
\textbf{Figure 5} shows the atomic number dependence of the transition energies theoretically calculated by the FAC code \cite{Gu2008}, along with optical $E1$ transition energies of Ag-like ions for comparison.
In the $Z$$>$60 region, Pd-like ions are not shown because they are not suitable for the present laser spectroscopy since the (4$d^{9}_{5/2}$5$s$)$_{J=3}$ level is not metastable due to the 4$d^{9}$5$s$ - 4$d^{9}$4$f$ level crossing \cite{Ivanova2009}.
In contrast to the typical electronic $E1$ transitions (e. g., $5s$  - $5p_{1/2}$ in Ag-like ions), the present $M1$ transitions with a number of inner-shell electrons show a gradual increment in the transition energy with an increasing atomic number.
As a result, in most regions where $Z$$>$30, transitions in either Pd- or Ni-like ions are available for laser excitation.

The present demonstration achieved precise determination of the transition energy with an uncertainty of $\Delta k$/$k_0$ $\simeq$ 3$\times$$10^{-6}$ for the $M1$ transition, which is inaccessible by emission spectroscopy due to the rapid $E2$ decay path from the upper fine-structure level.
From a technical perspective, we have succeeded in extending experimental targets in precision spectroscopy for trapped HCIs from spontaneously emitted transitions to non-luminescent transitions, providing a wider variety of spectroscopic targets.
This offers new opportunities, including the investigation of HCI clock candidates.
Prospects of the new type of atomic clock have also spurred developments in HCI laser spectroscopy with part-per-million uncertainties.
Several laser spectroscopic methods for forbidden transitions of trapped HCIs free from a systematic Doppler shift have been reported \cite{Mackel2011, Egl2019}.
These demonstrations employed a simple fine-structure transition $^2P_{1/2}$-$^2P_{3/2}$ in the doublet ground term of Ar$^{13+}$, whose transition energy is precisely known from direct wavelength measurements using passive spectroscopy \cite{Dragnic2003, SoriaOrts2006}, leading to recent quantum logic spectroscopy \cite{Micke2020, King2022}.
However, many potential candidates for the HCI atomic clock are not directly accessible using such passive spectroscopy because they possess complicated level structures with hyperfine splitting, and their clock transitions are not emitted in plasmas owing to their long lifetime.
Therefore, the extension of laser spectroscopy of HCIs to complex systems is a new challenge to overcome.
The present scheme can be applied to investigate the repump transitions and measure the hyperfine-structure constants of a clock state; otherwise is not accessible using passive spectroscopic methods.

Finally, we discuss the possibilities of other applications using the present spectroscopic technique.
The time-resolved LIF detection technique can be applied to hyperfine-level selective lifetime measurements without cascade contributions from higher levels, leading to deep investigations of hyperfine interaction \cite{Trabert2007} including hyperfine-induced-interference effects \cite{Yao2006} which have not yet been experimentally observed.
The demonstration of laser spectroscopy of forbidden transitions for HCIs in a laboratory plasma is expected to trigger the development of active sensing to investigate plasma conditions such as the plasma ion temperature and magnetic field, contributing to plasma diagnostics.

\section{Methods}
\subsection{Theoretical transition energy}
The transition energy between the fine-structure levels in 4$d^{9}$5$s$ is obtained in the framework of the multi-configuration Dirac-Fock (MCDF) calculation, combined with the relativistic configuration-interaction (RCI) approach, using the atomic structure calculation code package GRASP2018 \cite{GRASP}.
First, MCDF calculations were performed with an active space of single- and double-electron excitation from the 4\textit{s}, 4\textit{p}, and 4\textit{d} orbitals up to 8\textit{g}.
Each \textit{nl} orbital (\textit{n}=5-8, \textit{l}=\textit{s,p,d,f,g}) is added individually, with each outer orbital optimized while keeping all inner orbitals fixed.
Furthermore, to account for core-core and core-valence correlations with the inner orbitals, excitations from the  3$l$ ($l = s, p, d$)  orbitals were also included.
This active space treatment led to 3,300,000 $jj$-coupled configurations.
Moreover, corrections from the Breit interaction, that is transverse photon interactions in the low-frequency limit and QED corrections separating the self-energy and vacuum polarization corrections, are included in the RCI calculation.

\subsection{Theoretical hyperfine-structure constants}
Using the GRASP2018 code, we calculated the magnetic-dipole hyperfine-structure constant $A_{hfs}$ and electric-quadrupole hyperfine-structure constant $B_{hfs}$ for each fine-structure level ((4$d^{9}_{5/2}$5$s$)$_{J=3}$ and (4$d^{9}_{3/2}$5$s$)$_{J=2}$).
For the input values, the nuclear magnetic moment $\mu_I$ and nuclear electric quadrupole moment $Q_I$ were taken from \cite{Moment_Table}.
GRASP2018 also provides hyperfine-structure splitting calculations taking hyperfine-mixing with other fine-structure levels into account.
We compared two calculation cases, i.e. with and without considering shifts due to hyperfine-mixing.
It has been found that the resulting shift in energy for each hyperfine-structure level would be unobservable in the experiment.
Each correction for the hyperfine-structure constants was also evaluated using the same procedure as for the transition energy calculation.

\subsection{Estimation of uncertainties for the theoretical values}
There are several origins of uncertainties on the theoretically calculated values due to various corrections.
The uncertainties in the transition energy were estimated as follows:
The present MCDF-CI calculations involve valence-valence(VV), core-valence(CV), and core-core(CC) correlations.
They are considered by including configurations generated from all single- and double-excitations from the 3$s$, 3$p$, 3$d$, 4$s$, 4$p$, 4$d$, and 5$s$ orbitals to the active spaces (AS) of virtual orbitals.
Here we define four virtual orbital sets as follows: AS1 = \{$5p$, $5d$, $5f$, $5g$\}, AS2 = AS1 + \{$6s$, $6p$, $6d$, $6f$, $6g$, $6h$\}, AS3 = AS2 + \{$7s$, $7p$, $7d$, $7f$, $7g$, $7h$\} and, AS4 = AS3 + \{$8s$, $8p$, $8d$, $8f$, $8g$, $8h$\}.
We estimated the convergence with the size of the basis set by taking the difference between the transition energies calculated in the AS3 and AS4 stages ($\simeq$ 22 cm$^{-1}$).
We adopted this value for the uncertainty of the electron correlation calculation because additional correlations were not expected to exceed this convergence value even when more virtual orbitals we considered.
Another possible source of uncertainty is related to the calculated contribution from the Breit interaction.
The corresponding correction value was perturbatively computed in the RCI calculation through the exchange of a single transverse photon in the low-frequency limit \cite{GRASP, Chantler2014}.
Comparing the Breit contributions obtained from the perturbative approach to calculations in which the Breit term is included in a variational SCF process allows us to estimate the uncertainty due to the perturbative approach \cite{Koziol2020, Safronova2018}.
Previous studies have found that the magnitude of this effect is less than 0.3 ${\%}$ in the Ni-like case (among others) \cite{Koziol2020, Safronova2018} and that it is significantly reduced when the active space is expanded.
Here, we assume the maximum error owing to the perturbative treatment and adopt 0.5 ${\%}$ of uncertainty related to the Breit correction.
The resulting uncertainty is 2 cm$^{-1}$.
The QED contributions were smaller than the uncertainties related to correlation effects.
Thus, the resulting uncertainty associated with these terms was negligible.
The uncertainty in the Dirac-Fock term is caused by the uncertainty in the root-mean-square of the nuclear radius, which is insignificant for $^{127}$I  ($\simeq$ 0.008 fm \cite{Size_Table}).
The total uncertainty was calculated by applying the error propagation rule (quadratic summation) to individual sources of uncertainty.
This yielded an uncertainty of the theoretical transition energy of 22 cm$^{-1}$.
This uncertainty is strongly dominated by the electron correlation.
We also estimated the uncertainty for each $A_{hfs}$ and $B_{hfs}$ constant by employing the same procedure adopted for the transition energy.

\subsection{Simulation of the Zeeman splitting}
The Zeeman splitting for each hyperfine-structure level was calculated using the HFSZEEMAN95 package \cite{HFSZEEMAN,HFSZEEMAN95}, which is based on inputs from GRASP2018 \cite{GRASP}.
This calculation employs an accurate treatment of the intermediate field regime; therefore, the calculated splittings are reliable for a wide range of magnetic fields.
\textbf{Fig.~2~c} shows the differences in the Zeeman splitting between the initial and excited levels of the laser transition.

\subsection{Simulation of the transition intensities}
The hyperfine-structure-resolved Einstein $A$ coefficients were obtained by the summation of the Einstein $A$ coefficients for every $\Delta m_F = 0$ transition at each initial hyperfine-structure level.
The transition rate for an $M1$ transition between magnetic hyperfine-structure sub-levels $\Gamma^\prime m_F^\prime$ and $\Gamma m_F$ is given by
\begin{eqnarray}
\begin{multlined}
A(\Gamma^\prime m_F^\prime \rightarrow \Gamma m_F)\\
=\frac{2.69735\times10^{13}}{\lambda^3}\sum_{q}|\bra{\Gamma m_F}M^{(1)}_q\ket{\Gamma^\prime m_F^\prime}|^2,
\end{multlined}
\end{eqnarray}
where $M^{(1)}$ is the magnetic dipole operator, and $\lambda$ is the transition wavelength (in \AA).
Using the wavefunction expansion of the magnetic hyperfine substates,
\begin{equation}
|\Gamma m_F> =\sum_{\gamma,J,F}d_{\gamma,J,F}|\gamma I J F m_F>
\end{equation}
together with the Wigner-Eckart theorem (the dipole operator only acts on the electronic space, so we may decouple the nuclear and electronic parts in the reduced matrix element), equation (1) can be re-written as \cite{HFSZEEMAN95}
\begin{eqnarray}
\begin{multlined}
A(\Gamma^\prime m_F^\prime \rightarrow \Gamma m_F)=\\
\frac{2.69735\times10^{13}}{\lambda^3}\sum_{q}|\sum_{\gamma J F}\sum_{\gamma^\prime J^\prime F^\prime}d_{\gamma J F}d_{\gamma^\prime J^\prime F^\prime}\\
\sqrt{(2F^\prime+1)(2F+1)} (-1)^{F-m_F} \\
\begin{pmatrix}
F & 1 & F^\prime\\
-m_F & q & m_F^\prime
\end{pmatrix}
(-1)^{I+J^\prime+F+1}\\
\begin{Bmatrix}
J & F & I\\
F^\prime & J^\prime & 1
\end{Bmatrix}\bra{\gamma J}|M^{(1)}|\ket{\gamma^\prime J^\prime}|^2.
\end{multlined}
\end{eqnarray}
Here, $d_{\gamma J F}$ are the expansion coefficients, and $\bra{\gamma J}|M^{(1)}|\ket{\gamma^\prime J^\prime}$ is the reduced transition matrix element between the fine-structure levels.
The $A$ coefficients for all $M1$ transitions were calculated using the HFSZEEMAN95 package \cite{HFSZEEMAN,HFSZEEMAN95}.
Finally, we sum the Einstein $A$ coefficients for the $\Delta m_F = 0$ transitions of every $m_F$ sub-level and obtained the transition intensities $gA$ of the $M1$ transitions, as shown in \textbf{Fig.~2~b}.

\subsection{Fitting model}
We determined the hyperfine-structure constants $A_{hfs}$, $B_{hfs}$, $A_{hfs}^{'}$, $B_{hfs}^{'}$ and the fine-structure transition wavenumber $k_0$ using the following model equation to fit experimental data.
\begin{eqnarray}
\begin{multlined}
f(k) =\\
I_{0} \sum_{|F^{'}-F|\leq 1} gA_{F^{'}F} \exp(\frac{4\ln2(k-(k_{0}+k_{F^{'}F}))}{k_D^{2}}).
\end{multlined}
\end{eqnarray}
Here, it is assumed that each line profile is defined by a Gaussian function with the same line width because the hyperfine-structure splitting energies are significantly smaller than the fine-structure transition energy.
$k_D$ represents the Full-Width at Half Maximum (FWHM) of the transition line profiles.
For $gA_{F^{'}F}$, we employed theoretically calculated results for the relative transition intensities, as described in the previous section.
$k_0$ is the original transition energy between the fine-structure levels ((4$d^{9}_{5/2}$5$s$)$_{J=3}$ $\rightarrow$ (4$d^{9}_{3/2}$5$s$)$_{J=2}$).
$k_{F^{'}F}$ is the hyperfine-structure shift for each transition given by
\begin{eqnarray}
k_{F^{'}F} &=& k_{F^{'}} - k_{F}.
\end{eqnarray}
$k_F^{'}$ and $k_F$ are hyperfine-structure shifts from the original level for (4$d^{9}_{3/2}$5$s$)$_{J=2}$ and (4$d^{9}_{5/2}$5$s$)$_{J=3}$, respectively.
The hyperfine-structure splitting at each fine-structure level is given by
\begin{eqnarray}
\begin{multlined}
k_{F^{'}} =\\
 \frac{1}{2} A_{hfs}^{'} C^{'} + B_{hfs}^{'} \frac{\frac{3}{4}C^{'}(C^{'}+1)-I(I+1)J^{'}(J^{'}+1)}{2I(2I-1)J^{'}(2J^{'}-1)}
\end{multlined}
\end{eqnarray}
and
\begin{eqnarray}
\begin{multlined}
k_{F} =\\
  \frac{1}{2} A_{hfs} C + B_{hfs} \frac{\frac{3}{4}C(C+1)-I(I+1)J(J+1)}{2I(2I-1)J(2J-1)}.
  \end{multlined}
\end{eqnarray}
Here, $C^{'}$ and $C$ are given by:
\begin{eqnarray}
C^{'} &=& F^{'}(F^{'}+1) - J^{'}(J^{'}+1) - I(I+1)
\end{eqnarray}
and
\begin{eqnarray}
C &=& F(F+1) - J(J+1) - I(I+1).
\end{eqnarray}
Under the assumption of a Maxwellian distribution, the equation for the ion-temperature and spectral line width is given by:
\begin{eqnarray}
T &=& \frac{Mc^{2}}{8k_{B}ln2}(\frac{k_{D}}{k_{0}})^{2},
\end{eqnarray}
where  $M$, $c$, and $k_B$ are the particle mass, speed of light, and Boltzmann constant, respectively.
Equation (10) can be re-written as:
\begin{eqnarray}
k_{D} &=& \sqrt{\frac{8Tk_{B}ln2}{M}}\frac{k_{0}}{c}.
\end{eqnarray}
Equations (11) and (4) provide theoretical spectra.

\section{Data availability}
The data that support the findings of this study are available from the corresponding author upon reasonable request.

\section{Code availability}
The FAC code is available at https://www-amdis.iaea.org/FAC/, the GRASP2018 code at https://www-amdis.iaea.org/GRASP2K/, and the HFSZEEMAN95 code at http://dx.doi.org/10.17632/rv2vycs7pg.1.

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Minnesota Agencies
Information on Minnesota State Agencies, Boards, Task Forces, and Commissions
Compiled by the Minnesota Legislative Reference Library
Woman's Committee (Public Safety Commission)
Active dates:1918-1919
Public Safety Commission resolution
Function: The Woman's Committee concerned itself with food conservation, Americanization, child welfare or child "conservation," public health and social welfare, foreign relief, patriotic education, vocational training for women, and education in all aspects of home economics. Its Committee on Women in Industry cooperated with the state Department of Labor in conducting a survey of women employed outside the home, lobbied for the "Women's 8-Hour Bill," and generally monitored the situation of working women with respect to wages, hours, and working conditions. The state Woman's Committee supervised a network of district chairmen (from 10 congressional districts), county chairmen, town chairmen, and ward and block workers. It cooperated with or worked through many existing women's organizations.
History: The Woman's Committee (officially the Women's Division) was created by resolution of the Public Safety Commission on May 21, 1918, with the appointment of Mrs. T. G. Winter as state director, followed by the formation of an executive committee comprising representatives of major women's organizations and also of the state Board of Education, the state Department of Labor, and the University of Minnesota "Farm School."
The same committee was also authorized by the Council of National Defense to act as the Minnesota unit of the National Women's War Organization. It was sometimes also referred to as the women's auxiliary of the Minnesota Commission on Public Safety.
The committee closed its office in May, 1919.
Public Safety Commission
Membership: Original appointees: Alice Ames Winter (Mrs. Thomas G.), director/chairman; Miss Josephine Berry; Miss Agnes Peterson; Mrs. Edwin Stuhr; Miss Marian Vannier; Miss Annie Shelland; Mrs. Francis Buell Olson; Miss Caroline Crosby; Mrs. Elbert Carpenter; Mrs. Walter Thorp; Mrs. Bertha Allen; Mrs. W. T. Coe; Mrs. Bertha Dahl Laws; Mrs. W. R. Mandigo; Mrs. Charles P. Noyes; Mrs. Cordenio Severance; Mrs. George Squires; Mrs. J. L. Washburn.; Additional members; Miss Aimee Fisher, secretary; Miss Mildred Weigley; Mrs. James Swan; Mrs. John N. Jackson; Mrs. George H. Partridge; Miss Elizabeth Congdon.
Internet resource:
Minnesota Historical Society Finding Aid for the Public Safety Commission: Woman's Committee
Record last updated: 01/29/2016
Additional print information on this group may be available in the Library's collection of agency notebooks. Please contact a librarian for assistance. The Minnesota Agencies database is a work in progress.
Agencies Search
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Have you met Laura Versfeld?
Today, we're getting to know Laura Versfeld a little bit better! This is part of a series of interviews we will be having with KIKI members. If you would like to be interviewed go to our interview page and answer a few questions!
Although, now when I think about it, when I was younger, I did always have my parents camera in my hand photographing my cats outside on the grass… I guess the urge has always been there, I was just too ignorant to notice.
That's all I really need… If anything happened to my husband an animals, I think I would go crazy! But since there's time to grab two more things, I think I would grab my iPad and maybe something out the grocery cupboard – om nom nom!
Travel – where we wish to go and things we'd like to do… It's the most frequent conversation in the car when going somewhere.
Arrogance! Just typing it makes me angry! Also, people with no sense of humour – laughter is the best medicine people!
I would choose two tickets to Mombasa, Kenya – thank you very much:) And if she really wants to spend, an underwater housing for my camera too please!
I think it would be my Canon EF 70-200mm f/2.8 L IS II USM Lens – that beautiful white lens is awesome and cannot live without it (even though my 24-70 is also my fav!).
Around the world in 80 days and photograph it as we go:) Can you imagine?
I really love Jack Johnson, he's been my favourite since I was in high school. Then a combination of Dave Matthews Band, Foster the People and John Mayer.
Studio work is my least confident – I feel too restricted strangely.Most confident… hmmmm, not too sure. Portraiture, I think.
Go with the flow – I just take things as they come, mostly because I know my husband has things all planned out.
I would love to go to Mombasa, Kenya right now. I love the african vibes and friendly people – plus, their snorkeling and scuba is awesome!
This one – www.lvphotography.co.za/?p=1311 ! Because Jemma was gorgeous and full of smiles!


text:
Unboxing Helix Mattress: 6 Models Reviewed
December 23, 2018 by ksholloman
If you've ever been researching mattresses online, you know that finding a brand new bed-in-a box isn't always easy. For starters there are tens of thousands of companies competing to grab interest (give the benefit or leave it). And there are so many claims that making a decision on which mattress is most suitable is a challenge. Unboxing Helix Mattress
To start limiting the options available, pick a mattress online that has a high reputation for quality and then look through their models to see whether any can be a good fit. Helix is a fantastic starting point. The reputable online mattress maker has a variety of mattresses that are designed to appeal to a variety of sleepers. In this Helix mattress selection, there's a good chance you'll find the right mattress to suit your needs!
What Helix mattress will be the right option for you? To discover the answer, read on for our comprehensive Helix Mattress review!
Helix became famous because it was one of first mattress manufacturers to offer fully customizable mattresses. This included mattresses with two distinct constructions on either side to accommodate couples with different preferences for sleeping. While the company recently slashed its customized products, it is still committed to supplying a wide selection of mattresses for sleepers.
Helix now includes six different hybrid mattress in its lineup that have a distinct hardness degree and plushness level. Here's a rundown of who's most likely to sleep on these mattresses (and those who may not).
People who require a large number of options to choose from
The six Helix models that comprise the main range cover a wide range of firmnesses, providing you with many options for finding the perfect mattress. (You can change one of these models to an LUXE model, and Helix also has an extra-firm mattress specifically designed for heavier people, Helix PLUS. Helix Plus.) Here's a short breakdown of how the major models compare in terms of suitability for different sleeping position.
You might have noticed that stiffness has already been discussed within this list. That's because one of the most important aspects to think about when buying for a new mattress is the firmness (and how firmness affects comfort). These factors will tell you a lot about a mattress's suitability for your chosen sleep place (s). Let's review of the comfort and firmness that comes with the Helix mattress range.
The Helix mattresses are available in a variety of hardness options, with the most soft being moderately soft, and the firmest being fairly firm. Its Helix Sunset is on the lower end of the scale We gave it a hardness rating at 5.5 /10 on the scale of firmness. (A 6.5/10 would be the industry standard for medium firmness.) Helix Dusk is next. Helix Midnight is next, and we gave it a score of 6/10 which means that it's softer than normal. The Helix Midnight as well as the Helix Dusk are in the middle of the spectrum. Both mattresses scored approximately a 7/10 which is slightly more firm than the average. They are Helix Twilight, as well as Helix Dawn are at the harder end of the spectrum, both getting an 7.5/10 score (firmer than average).
It's crucial to be aware that the level of hardness is a matter of individual preference. If you're looking for the firmness, you could evaluate these mattresses in different ways based on your body weight and your personal preferences. People who are heavier, for instance could find the mattresses more firm as they can push further into the mattress and reach into the support layers. On the other hand, people who weigh less discover that these mattresses are more supple due to their position on the comfort level of every bed(s).
We slept on the Helix mattresses for a lengthy period of time in order to gain a clear picture of what it's like to rest on each model in various positions. Have a look at the results!
Due to its softness because of its softness, Helix Sunset didn't feel nearly supportive enough for back sleeping. Our hips were a bit too far in the bed, causing the spine to become misaligned.
While the Helix Sunset's softness isn't ideal for those who sleep on their backs but it's great for side sleepers. We were very at ease in this position due to the soft mattress cushioned possible stress points around the hip and shoulder. In actual fact, it's one of the best mattresses to relieve hip discomfort we've seen.
The Helix Sunset is not supportive enough for stomach sleeping because of its softness. Our hips sank too deeply into the mattress and pulled the back out of position just the way they did when were sleeping back to back.
As a back sleeper while sleeping, back sleeping, the Helix Moonlight was adequate but not outstanding. If you're planning on sleeping in this position for the duration of the through the night, you'll require a mattress with additional support and helps maintain an appropriate spine alignment.
It is the Helix Moonlight is an excellent choice for side sleeping because of its comfort. We didn't feel any uncomfortable pressure around the hips or shoulders.
It is the Helix Moonlight, like the Helix Sunset, is not supportive enough for stomach sleeping. Our hips fell too deeply to the bed, which caused the spine to shift.
When we lay down upon the Helix Midnight and feeling fantastic, we were able to feel great. We enjoyed a touch of pressure alleviation without sacrificing spinal alignment thanks to the mattress's excellent balance of support and comfort. It's the most comfortable mattress for back sleepers on this list.
Although the Helix Midnight is more firm in comparison to the Helix Sunset as well as Moonlight and Moonlight, we were able to rest comfortably on our sides on this mattress. It provides adequate pressure alleviation on the hip and shoulder, in our opinion.
When we slept with our stomachs on the Helix Midnight, we were good but not great. People who sleep in this position all night should look for a firmer mattress that provides greater spinal support.
The Helix Dusk is more supportive than the other models that we've tested. This could explain why we felt so at ease while sleeping on our backs. We're sure that we'll be able to maintain an ideal spinal alignment throughout the night because of the mattress's supportive qualities.
It's probably not surprising it is that Helix Dusk feels a little too firm for a side sleeper considering that we've moved to the more firm end of the spectrum. We felt some pressure around the shoulder and hip that would create a lot of discomfort if you slept in this position all night.
The Helix Dusk should suit stomach sleepers who weigh around average since it can help to maintain a healthy spine alignment. However, stomach sleepers who are heavier may not receive enough support here.
The Helix Twilight was proved to be the best mattress for back discomfort. It is ideal for those who require extra support due to increased weight, back pain, or other causes. The firmer construction of this mattress assists in keeping the hips elevated and aligned with the spine.
Since the Helix Twilight is slightly firmer than other mattresses, we found it difficult to lay on our backs on the mattress. We felt suffocated in the hips and shoulders.
For most stomach sleepers, the Helix Twilight mattress to be a great fit, since the mattress's hardness will provide enough of spinal support in this position.
Back sleepers who like mattresses that are firm will appreciate the Helix Dawn's high level of support. However, those who like a little pressure alleviation when resting on their backs may likely find this mattress to be excessively firm.
The Helix Dawn is far too hard for side sleeping and you'll be left having a lot of pressure points around your shoulder and hip. A softer model will be much more suitable for those who sleep on their sides.
It is the Helix Dawn mattress is considered to be the most comfortable mattress designed for stomach sleepers in our opinions. In the evening this supportive and firm mattress will keep your hips up and in alignment with the spine.
Helix mattresses are all hybrid structure that has foam layers over coils. However, despite these similarities every Helix mattress has its own distinct personality.
The Helix Sunset offers a soft top and a well-balanced foam feel. The soft comfort layer allows sleepers to relax and provides the mattress with a slow-moving feel.
The Helix Midnight, like the Helix Sunset, has a balanced feel and a slower-moving upper layer. The Midnight is firmer than the Sunset which allows sleepers to sink more deeply into the top layer.
The Helix Dusk is solid and bouncy. This is because of the use of high-performance foam for the layer on top, and coils in the layer supporting it.
It is similar to the Helix Twilight, like the Helix Sunset and Midnight, is characterized by a slower-moving top. It's still a solid mattress despite the comfort layer being slightly more comfortable.
Helix Dawn, like the Helix Dawn, like the Helix Dusk, has a soft, firm and bouncy feel it because to the use of dynamic foam (in the cushion layer) and coils (in the support layer).
It is the Helix Midnight (which combines spinal support and pressure reduction) or Helix Dusk (which combines pressure reduction and spinal support) or Helix Dusk are likely to be preferred by average-weight back sleepers (which provides a more firmer spine support).
The Helix Late at Night (if your preference is a more firm feeling) or the soft and more pressure-reducing Helix Moonlight (or Sunset) is most probable for average-weight side sleepers.
The stomach sleepers who are with a moderate weight should choose the supportive Helix Twilight or Dawn.
The Helix Dusk should provide appropriate support for heavyweight back sleepers, as it relieves pressure while maintaining the alignment of the spine.
The stomach sleepers who are heavy On the other hand tend to go towards the Helix Dawn (the firmest mattress in the collection) for the best spinal support.
There should be a wide range of options for light back sleepers: The Helix Moonlight, Midnight, and Dusk all offer plenty of spinal support as well as different degrees of pressure relief that can accommodate various sleeping styles.
Similar to the side sleepers that are lightweight, you can select from Helix Midnight, Moonlight, or Sunset that should all provide adequate pressure relief and allow users to adjust the level of hardness according to their requirements.
Finally, stomach sleepers will find Helix Twilight or Dawn to be the most supportive. Helix Twilight and Dawn as the most comfortable.
As far as construction is concerned, each of all of the Helix mattresses are built in the same way: They share the same cover and the foam comfort layers are laid over individually wrapped supports for coils.
Every Helix mattresses, in particular, have a SoftTouch Design cover that is flexible, soft and breathable. This design allows air to circulate freely through the mattress's top. Meanwhile, each Helix model has a support layer made up of individually wrapped coils that are stacked over a dense base foam which provides the mattress with it's overall design and stability.
The similarities end there for the most part. The foam layers that provide comfort differ in their thickness, stiffness, arrangement and kinds of foam. Additional materials are also offered on certain versions. Let's take a take a closer look!.
The Helix Sunset's comfort layer is made up of pressure-relieving Memory Plus Foam, which provides the slow-moving, comfortable feel of memory foam that it is known for. A transition layer composed of Helix Dynamic foam, a latex-foam replacement that's more firm, bouncier and more bolstering, sits under memory Plus Foam.
While the Sunset's top comfort layer is comprised out of Memory Plus Foam, the Helix Midnight's comfort layer and transition layer is made of the Helix Dynamic Foam. This is another latex-foam option and the numerous layers of this foam give it a bouncy feeling when compared to the Helix Sunset.
Memory Plus Foam is the primary comfort layer of the Helix Midnight, and it provides pressure reduction and body shaping. A transition layer of thick, high-grade polyfoam sits beneath that Memory Plus Foam. The layer is extremely flexible, meaning that the mattress in general responds to pressure more quickly.
The Dusk's main comfort layer is made up out of Helix Dynamic Foam, a latex-foam substitute that's bouncy and receptive. The layer is made comprised of Memory Plus Foam sits beneath the Memory Plus Foam layer. (Think about the Dusk's structure as similar to the one of that of the Helix Sunset, but reversed.) Helix Dynamic Foam has been laid over Memory Plus Foam to produce a bouncy, responsive surface, while Memory Plus Foam helps relieve pressure as sleepers sink deeper into the mattress.
Helix Twilight, like the Helix Twilight, like the Helix Midnight, has a slow-moving Memory Plus Foam layer above the dense, high-quality polyfoam layer that acts as a transition. Its Memory Plus Foam adds some convenience, but don't get fooled: this is a firm mattress with only a little bounce.
Then, last but not least The Helix Dawn has the Helix Comfort Layer made of Dynamic Foam that is layered over a high-quality, dense polyfoam layer transition layer. The result is an extremely firm, bouncey, and comfortable sleep surface with very little give.
When it comes to the size and cost for size and price, the Helix mattress collection offers a variety of variants. Check out the table below to see the cost of an Helix can set you back.
We tested the Helix mattresses to a set of tests to find out how well they performed in key areas such as temperature control, motion transfer, edge support and much many more. Read on to learn the results!
Are you sleeping hot or cold? If you're still concerned about the possibility of overheating, think about purchasing a LUXE version of your mattress.
According to our tests certain models are better than other models when it comes to keeping out any disturbances that might occur on the surface of the mattress. It was found that the Helix Sunset, Midnight, and Twilight provided the best motion-seclusion. That's because they have a memory foam that is slower moving close to the top of each of the models, it does well at absorption of motion. These are among the best mattresses for couples on the market.
Every Helix mattress provided an excellent edge support across all models. When we sat and slept at the edge of each model, we felt comfortable and safe.
The Helix mattresses are made from high-density foams as well as sturdy coils which ensure that they can last for a long period of.
We noticed the off-gassing of the six Helix mattresses in the beginning. It will disappear in a few days, in the event that it is not earlier.
There was no noticeable noise when we moved around on one of these mattresses during the time we wrote our review. However, because all of them have coils, it's possible that they'll start to sound squeaky over time.
If you are looking for a sexual mattress, most individuals are concerned about how easy it will be to move places on their mattress. Since all Helix mattresses are made of coils, they should be responsive enough to allow you to move around easily on each. The models with memory foam on their top layers (particularly those that have memory foam in the top layer (such as Helix Sunset, Midnight, and Twilight) could make changing positions a little more difficult because of their slow motion.
A 100-night sleep trial and a 10-year mattress guarantee are provided in every Helix mattress.
Are you looking for other queries? The frequent questions about the Helix mattress range have been answered!
Is Helix a suitable choice to make a bed?
Yep! Helix is well-known for its high-quality mattresses in a number of designs to fit a variety of kinds of sleepers. Your preferred sleep position(s) and other sleep requirements will determine the most suitable option for you.
In the case of Helix mattresses, how long do they last?
A Helix mattress can't be turned. The support layer beneath in place of the cushion on one of these mattresses can result in an extremely uncomfortable mattress.
You may purchase Helix mattresses directly on their website, however for more value, you can look through our Helix coupons and promo codes! Unboxing Helix Mattress
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Unboxing Helix Mattress
Helix Mattress Clone: 6 Models Reviewed
Helix Sunset Luxe Mattress Review: 6 Models Reviewed


A lot of entrepreneurs are ignorant about the consequences of debt and they continue to apply for loans until they land up in a huge financial crisis. Statistics suggest that no matter how small or big the organization is, the burden of debt can bring them down.
However, entrepreneurs should analyze their financial condition in right time so that they can avoid any unwanted and threatening situation. Business owners should adopt suitable business strategies and customize daily activities so that they can remain afloat in this highly competitive market. Thus, take a look at some important aspects that can be helpful to manage a business in difficult times.
Engaging in many charitable works can help an organization to grow its reputation, but at the same time, such kinds of activities are considered for tax deductions. Thus, it is very important for an organization to keep all donation related document and receipts safely so that it can be submitted to the tax department. Here are a few examples of privileges that can be enjoyed by an organization for running charitable activities.
Relying much on a useless business budget is one of the primary causes of financial debacle. Business entrepreneurs who have certain objectives and goals should prioritize and modify existing budget plans and should eliminate all bad and inefficient virtues that can bring negative results.
However, the newly prepared budget should focus on areas such as valuating the cost of equipments, production marketing, and other expenses. Another aspect is that an entrepreneur with credit card debt should pay more than their actual assured monthly payment so that they can recover all their debt long before their scheduled time.
Indebted people are well aware about the fact that business loans always carry high interest rate that often falls heavily on the business. However, prioritizing the present debt and its repayment system can reduce the stress associated with it. Entrepreneurs should free up a good amount of cash for their debt repayment. By following the process of repayment system properly, an entrepreneur can establish good credit history, which is a very important aspect for an organization.
Many terms and conditions are associated with business debt and it is not possible for a businessperson to handle those things alone. Many debt management agencies are available in the locality and even online that provide experienced advisors with much affordable fees.
Professionals who are working in the national debt relief agencies are qualified enough to advise people who are in need of suggestions. Several programs such as debt consolidation, debt settlement, or debt management are available that can offer huge relief for indebted entrepreneurs.
Let the debt relief agency assesses your financial condition and see how they can bring the best debt relief program for your business. You should know that a reputed debt solution agency always features experts who will be at their best while negotiating with your creditors so that they can prepare a convenient and affordable debt relief plan. However, before dealing with any such agencies, make sure that the Better Business Bureau has rated it.
Author Bio- Julian Whitmore is debt management expert who has been working for a debt relief agency for more than ten years. Along with this profession, the author writes for many national debt relief agencies to help people and entrepreneurs get out of debt burden.


&TV's popular weekend reality show 'The Voice India – Kids' Season 2 has come to an end with the young star, Manashi Sahariah who rocked the stage under the guidance of Coach Palak Muchhal, being crowned the winner!
With the competition getting tougher each passing week, the top six contestants who battled it out till the end were Manashi Sahariah, Shekinah Mukhiya, Guntaas Kaur, Mohammad Faazil, Shruti Goswami and Neelanjana Ray. However, it was Manashi who not only lifted the winner's trophy but also took home a cheque of Rs. 25,00,000/- as coach Palak rejoiced in jubilation. Nilanjana was the first runner up while Shruti was the second runner up of the season, and were awarded a cheque of Rs. 10,00,000/- respectively. All the Top six contestants were awarded gift hampers from Cadburys by Mr. Amit Shah, Associate Director, Marketing – Gum, Candy and Beverages, Mondelez India.
Hailing from a small district in Assam, Manashi picked up singing from a tender age of 3 while listening to her mother humming. Since then, there's been no looking back for her. Back in her hometown, Manashi found it difficult to find someone who could train her and provide guidance in Hindi music. However, this didn't burn her spirits and soon after Manashi started listening to and watching Hindi videos online through which she improved her skills further. However, it was her village, all of 300 people, who came together to organize funds so that Manashi could get the opportunity to travel to Mumbai and participate in The Voice India Kids. And all their efforts have paid off today as she heads home soon with the winner's trophy.
The Grand Finale of 'The Voice India – Kids' Season 2 on &TV was a spectacular coming together of talent and the Coaches – Palak Muchhal, Shaan and Himesh Reshammiya. Adding a whole lot of fun to the evening were the quirky awards which were rolled out not just to the contestants but the coaches and the families alike.
Next articleRanveer Singh & Aditya Chopra meet to discuss next?
Papon to miss shoot of 'The Voice India' next episode?


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Effect of osteopathic manipulative treatment on incidence of postoperative ileus and hospital length of stay in general surgical patients
J Am Osteopath Assoc
CONTEXT: Postoperative ileus is a known complication after abdominal operations, and the clinical efficacy of osteopathic manipulative treatment (OMT) in postoperative surgical patients has seldom been the subject of research. OBJECTIVE: To determine whether there is a relationship between postoperative use of OMT and postoperative outcomes in gastrointestinal surgical patients, including time to flatus, clear liquid diet, and bowel movement and postoperative hospital length of stay (LOS). DESIGN: A retrospective cohort study. SETTING: A 350-bed urban community hospital with an osteopathic residency program in general surgery. PATIENTS: Fifty-five patients who underwent a major gastrointestinal operation, who did not die, and who had complete perioperative medical records. MAIN OUTCOME MEASURES: We evaluated demographic data; American Society of Anesthesiologists physical status class; preoperative comorbid conditions; postoperative complications; postoperative time to flatus, clear liquid diet, and bowel movement; postoperative hospital LOS; electrolyte abnormalities; and types of narcotics used. RESULTS: Of the 55 patients who met the study criteria, 17 had received postoperative OMT and 38 had not. The mean age was 60.3 years in the OMT group and 62.1 years in the non-OMT group (P=.70). The 2 groups were similar in terms of American Society of Anesthesiologists class, number of comorbid conditions and of postoperative complications, presence of electrolyte abnormalities, and narcotic use. The time to bowel movement and to clear liquid diet did not differ significantly between the groups. The mean (standard deviation [SD]) time to flatus was 4.7 (0.4) days in the non-OMT group and 3.1 (0.6) days in the OMT group (P=.035). The mean (SD) postoperative hospital LOS was also reduced significantly with OMT, from 11.5 (1.0) days in the non-OMT group to 6.1 (1.7) days in the OMT group (P=.006). CONCLUSION: Osteopathic manipulative treatment applied after a major gastrointestinal operation is associated with decreased time to flatus and decreased postoperative hospital LOS.
Baltazar, Gerard A Betler, Michael P Akella, Krishna Khatri, Rishi Asaro, Regina Chendrasekhar, Akella eng Comparative Study J Am Osteopath Assoc. 2013 Mar;113(3):204-9.


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Q: Upgraded to snow leopard and can't install git from macports [architecture mismatch error] I've upgraded to Snow Leopard, re-installed XCode, re-installed macports and when I try to install git I get:
:~ $ sudo port install git-core +svn
Error: Cannot install git-core for the arch(s) 'x86_64' because
Error: its dependency zlib is only installed for the arch 'i386'
Error: and the configured universal_archs 'i386 ppc' are not sufficient.
Error: Unable to execute port: architecture mismatch

Am I doing something wrong?

A: My first answer: it looks like the issue is with zlib. I'm guessing you have an old (pre-Snow-Leopard) version of zlib installed; port is seeing that it's there (and therefore not installing a new version) but isn't seeing the right architecture to build a 64-bit Git. I'd uninstall and reinstall zlib within port first, then try git again.
My second answer is a cop-out: try installing Git from the installer instead. (That's what I was trying to do.)


The Chicco MyFit� harness/belt-positioning car seat is designed to grow with children from toddler through big kid with easy transition from five-point harness to vehicle seat belt. Nine headrest positions accommodate growth throughout both modes and work together with a four-position recline to support proper posture. An extra-deep ErgoBoost� seat with dual-density foam padding is sloped and contoured for superior comfort.
DuoGuard� side-impact protection offers two layers of protection for two zones with a rigid shell and EPS energy-absorbing foam that surround the head and torso. The seat shell is also reinforced with a steel frame for superior impact protection.
From the makers of the #1-rated KeyFit� and NextFit�, the MyFit� is designed with smart functionality that makes it the easiest to install simply, accurately, and securely, every time. A four-position ReclineSure� leveling system and RideRight� bubble levels help achieve and verify proper angle in the vehicle seat. Premium LATCH connectors and a LockSure� belt-tightening system with wide routing make it easy to achieve a tight and secure fit with LATCH or the vehicle seat belt.
A padded, no-rethread harness with a one-pull tightener provides reassuring security for growing toddlers. The harness easily hides away to create a belt-positioning booster with shoulder and lap belt guides for big kids four years and up. Two dishwasher-safe CupFolders� feature easy push-button removal and fold out of the way to save space when empty.
Happy parents and happy kid!
Luxurious, comfortable fabric. Extremely easy install with shoulder belt lockoff. One of the slimmest HBB with multiple reclines. All around amazing seat. We are beyond happy with our purchase. Great job Chicco!
Excellent car seat for my 2.5 year old! I have a tall but tiny one who wants to �€œdo it herself�€, so that�€™s what prompted my move from the Nextfit to the Myfit. She feels like she�€™s in a big girl seat with all the comforts of a booster seat, but with all the safety of Chicco and a 5-point harness. I love that this will be the last seat she'll ever need. Not as cushy as the Nextfit, but still uses the memory foam for cushion. It looks great, isn�€™t bulky (like our Britax Frontier), and for the price this is a great seat! When comparing to the Frontier, the install still requires you to crawl in and out of the seat for a proper install, so Britax Clicktight still holds the �€œeasiest install�€ award, but my DD seems just as comfy in her Chicco. Very, very easy to move height up and down! I love that it has multiple recline positions, so my daughter's head won't slouch forward when she falls asleep.
I�€™ve tried other car seats, but I always go back to chicco. My daughter has gone 3 already. Now 5yrs old we upgraded her to the MyFit and as expected it�€™s a great car seat. Easy to use, to install, elegant and above all very comfortable.
easy to install. Fits on my 3rd row of my Toyota Highlander. Love the design and easy to remove cup holders for cleaning. Doesn�€™t take up much space.
My daughter seems comfortable and even though we haven�€™t had a long road trip. She hasn�€™t complain after 4 hours drive.
My son wouldn�€™t stay put in regular booster seat so we had to switch back to a harness belt...he loves this seat! It�€™s very comfortable and we love that it declines as well. It doesn�€™t make him feel like he�€™s in a baby car seat yet provides the safety we need! Very happy customer!!
This seat is so much more comfortable than any other one we�€™ve tried. They are practical and functional! We love them!
We have always had Chicco car seats, so when I came accross this, I had no doubt we�€™d love it! We were just going to start forward facing our four year old and wanted something that was easy for her to get in and out of by herself. She got to pick her color, and she loves it as well!
I�€™ve had Chicco safety seats since my son was born. With his new brother, we wanted to move him to a booster and use the Nextfit for the baby. After a lot of research I decided on the MyFit. The secure 5 point harness and classic Chicco install options made it an awesome fit for him. He�€™s 5.5 years old and loves it! He�€™s even mastered buckling himself in with it.
This car seat is comfortable. Super easy to install! I love that the latch is easily store away in the seat base. Cup holders are awesome and handy since they can be squished. I have this is the center seat of my highlander next to a maxi cosi rear facing with my 1.5 yr old. It does carry over a bit to the other seat in that row but I think it�€™s more because of the infant seat than this one. Overall super happy to find a comfortable easy to install harness to booster so I can keep my daughter in the harness as long as possible. Safety is big for me and this seat is perfect!


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Home review Kohinoor Malayalam Movie Review, Rating, Box Office Collection
Kohinoor Malayalam Movie Review, Rating, Box Office Collection
Kohinoor, a pure suspense movie which stars Asif Ali, Indrajith, and Vinay Forrt in the lead roles. The movie is directed by Vinay Govind (Kil Poyi fame) and jointly penned by Salil Menon and Ranjeeth Kamala Shankar.
Kohinoor is produced by Asif Ali, Sajin Jaffer and Brijeesh Mohammed under the banner Adam's World Of Imagination.
Jeethu Joseph - Dileep team-up "Life Of Josutty" is running without twists and here "Kohinoor" came up with several twists at end point, that steals the show.
Louis (Asif Ali) is a happy-go-lucky guy who has a strange admiration for the underworld dons. He is highly fascinated by Mohanlal's character Vincent Gomez from the popular movie Rajavinte Makan, and wants to be a smuggler like the character. Louis's best friend is Aandy Kunju (Aju Varghese). Later, Louis and Aandy meet Haider (Indrajith), who works for Mumbai underworld and Freddy (Vinay Forrt) and Nicholas (Chemban Vinod Jose), who comes from Kochi. The trio has a secret mission and Louis joins them. Meanwhile, Louis falls in love with Daisy (Aparna Vinod), a sales girl. As the movie having a bunch of twists and turns, we not revealing much over here in story side...so just go to theater and feel the value of "Kohinoor".
After a long time, Asif Ali delivers an exuberant performance as Louis; but tends to over-act at some portions, by trying to make his acting and style as more classy like 90's actors.
Aju Varghese, who appears as Aandy Kunju, is at his usual best. Vinay Forrt, and Chemban Vinod Jose, who Freddy, and Nicholas are perfect in their roles and makes a great combo. But the real show-stealer of the movie is Indrajith, who plays Haider. The actor stuns with his terrific dialogue delivering skills and extraordinary screen presence. Aparna Vinod, who plays the female lead, is impressive in her minimal role. But the actress lacks an on-screen chemistry with Asif Ali; which badly affects the romantic track. Bhavana, who appears as Louis's ex-girlfriend Lilly, adds an extra flavour of entertainment to the film. The rest of the star cast including Mamukkoya, Saiju Kurup, Sudheer Karamana, Pradeep Kottayam, Bhagath Manuel, Biju Kuttan, Harikrishnan etc are perfect in their roles.
Performance Backbones
The movie is directed by Vinay Govind. It is evident that Vinay has the potential to make the real funny situations in his films; but he somewhere loses the control over the movie in first half and later it get back into a worthy watchable.
Pradheesh M Varma's cinematography has played an instrumental role in making an original ambience for the movie, which revolves around the 80's period. Arju Ben handles the editing, it is perfect. Ajay Mangad, who handled the art direction and Sameera Saneesh, who designed the costumes deserves a special mention.
Songs and Background score are composed by Rahul Raj. BK Hari Narayanan pens the lyrics. The song Hemanthamen provides the real nostalgic feeling; while Dum Dum Dum turns out to be an interesting fast number.
The right mixture of suspense, humour, thrill, nostalgia an over flowing twists and turns.
Rating : 6.5 / 10
TAG box office collection MALAYALAM review
box office collection MALAYALAM review


Alice was born to Lee and Sarah Russell Harris on October 8, 1875. She grew up in the Eldorado Community in Montgomery County, NC. In 1880, she lived with her parents. She had a brother who died at 6 months old in December 1877. Her mother, Sarah, died and Lee soon married again and had several children. His second wife was Nancy Elizabeth Russell. With Nancy, he had Bulah, Travis, Silvia, Oscar, Jessie, and Georgie.
On 25 April, 1894, she married William Christopher Harris.
By 1900, she's living with her husband and 2 children. Still in Eldorado. They're renting and he's a day laborer.
In 1910, she and William are still living in Eldorado. He's a laborer doing odd jobs. They still rent and they have 7 children; Jonah, Sarah, Clifford, Nina, Mattie, Joe, Iola. My grandmother, Racie, would come in June of the following year. By January of 1912, Alice is dead.
Her children went separate ways and William visited from time to time. He suffered from mental illness and committed suicide in 1924.
My grandmother went to live with Alice's parents. And now to the reasons I think my grandmother was right about Alice's name. Even though she never knew her mother, she did grow up with her grandparents. Her grandfather, at least, was one of the two people who named Alice and did all they could to help her know her mother. They would most certainly know Alice's name.
Virgillia is such an odd name. I've often wondered where it came from.


The Serial Data Transfer section allows the user to transfer serial digital data to the Modulation Input for Frequency and Phase shift keying schemes. The transfer size is from one byte to 512K bytes. The data may be looped from start to finish for bit rate testing from a single file or multiple files in a control sequence from applications like LabView.
DATA TRANSFER MAIN MENU - The main menu for this dialog allows the user to Load and Save data files or create a new file. All data loaded or created is placed in the working array buffer until the user transfers it to the on board SRAM by the Write to SRAM button.
CURRENT FILE - This is the current data file loaded in to the working array buffer displayed with its full path.
STORE DATA to ARRAY - The Store DATA to ARRAY Button allows the user to edit current data or create new data in the working array.
WORD COUNT SETUP - The word count allows the user to select a desired word count from the array. This function works with the SRAM starting address in order to allow a windowed data transfer from the array. This allows the user to store several frames in SRAM and select the frames desired for the test.
TRANSFER MODE SETUP - The transfer mode setup allow the user to select a SINGLE WORD, SINGLE BLOCK, or FULL BLOCK transfer. The word size is also variable from 1 to 16 bits. The user may also select the start and end bit in the word allow word windowing as well. The transfer mode also allows the user to control the bps rate of the transfer by controlling the reference frequency and rate divider.
STATUS OF LAST COMMAND - This is a monitor field for the status of the last command executed in the dialog.
TRANSFER DATA - This is where the data is transferred to the active core of the PMG-130. The SINGLE and BLOCK transfer buttons allow the user to control a single word transfer or and entire block (word count) transfer.
HELP - This Button will activate the About dialog box and allow the user to select the online manual for help.
LOAD MODE & SERIAL DATA REGISTER - These buttons insure a relative starting point for the data transfer.
DATA LOOP CONTROL - This section is for diagnostics. It allows the data in the array to be looped indefinitely or to a specific loop count.
SRAM START ADDRESS - This is the starting address in the SRAM of the data to be transferred to the active core.
DATA IN CURRENT ARRAY - This is the current working array data window that will allow the user to verify and edit the data prior to transfer.


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Comics/Graphic Novels
Bitch Planet Triple Feature Series Exists In a Parallel Non-Compliant Universe
Karama Horne Sep 6, 2017
This is a guest post from Karama Horne. Karama is the creator of theblerdgurl.com where she provides commentary, reviews and interviews on comics, sci-fi and geekdom from a "black nerd girl" perspective. She has been quoted on popular media sites like Comics Alliance, Comic Book Resources and The Beat. She also has been featured on panels at New York Comic Con, Awesome Con and The Schomburg Black Comic Book Festival. Follow her on Twitter @theblerdgurl.
Kelly Sue DeConnick and Valentine De Landro's Bitch Planet is probably the most feminist, satirical, diverse, and visceral story that I've read in awhile. The series, described by DeConnick herself as a "dystopian sci-fi take on the exploitation genre," started off in December 2015 and has published 10 issues (and two trade paperback volumes) to date. Taking a brief break from the series, DeConnick and De Landro decided to create an anthology series, recruiting other artists and writers to contribute to the series.
Not only has Bitch Planet won numerous awards and legions of fans, but the property has included futurists, feminist writers and scholars in the short stories, think pieces, and interviews that are featured in every issue at the end of the comic. Artist Lauren McCubbin has created some of the coolest retro backpage ads I've seen since I was a kid rummaging through my friend's dad's comic book stash.
In the original series, society is run by the Protectorate, a right-wing political group of megalomaniacal men who call themselves the Fathers. In this patriarchal society, women can be arrested or incarcerated for even the most minor of offenses, such as being overweight, gay, too smart, childless, or in one woman's case, simply being unwanted. Offenders or those who defy the law are considered "Non-Compliant" and are shipped off to an off-world penal colony called the Auxiliary Compliance Outpost, nicknamed "Bitch Planet." There, they are subject to assault by the prison guards, verbally abusive "therapy," and are made to battle against each other for sport in a kind of off-world prison Fight Club. But they are fighting back.
Bitch Planet: Triple Feature brings us three stories created by three new teams of writers and artists in each issue that all plausibly take place within the world of Bitch Planet, but just outside of the main arc. In Windows, written by Cheryl Lynn Eaton and Maria Fröhlich, a female guard at the prison is fired when a prisoner dies on her watch, and ends up working as a maid for one of the Fathers who watches the prison's drone feed for entertainment. In This Is Good For You by Danielle Henderson, Rowe Stein, Ted Brandt, and Clayton Cowles, a woman invites her friend to see a movie that turns out to be a propaganda film. In it we see one of the tactics used on female members of society outside of the prison. Taking plays right from a '50s etiquette handbook, women are told that their purpose in life is to be thin, have babies, and take care of the home. All notions of work and leadership are shunned because non-compliance is unacceptable.
Most of the Triple Feature stories are told in the not-so-distant future, which make them eerily plausible, like Those People by Alissa Sallah and Alec Valerius. This narrative demonstrates how even well-meaning law enforcement can commit horrible acts when indoctrinated with fear and bias. When the inadvertent massacre of a house full of LGBTQ partygoers leaves a combatant visibly shaken, his actions are written off as "pre-emptive self-defense." That concept, in this day and age, is so plausible in fact that it terrifies me.
In Without and Within by Andrew Aydin and Joanna Estep, a young woman is set up for failure in a at her first day on the job at a Trump-esque firm as she has to simultaneously figure out a new computer system to print a speech for her boss, and fend off the sexual advances of her boss's partner…whose actions said boss had clearly sanctioned.
I think the piece that punched me in the gut (albeit unintentionally I'm sure) was What's Love Got to do With It by Jordan Clark and Naomi Franquiz, in which a curvy thirty-something Latinx woman puts herself through an hilarious yet horribly disrespectful set of dates in order to quickly find someone to marry so that her parents won't be hit with a government "Old Maid Tax" which would force them to lose their home.
If that law were real, my parents would've been homeless.
As one would expect, these stories are multilayered and, like the rest of the Bitch Planet series, uphold the white het cis male concept of femininity and condemn female choice, careers, and independence as "threats to the patriarchy." Although there is struggle and often death, there is also perseverance and triumph as well.
DeConnick and De Landro's commitment to diverse writers and intersectional feminism is also to be commended here. In every issue I'm seeing names that are new to me or to this medium, and I'm happy that these artists are getting a chance in the spotlight. However, as with most anthologies, I'm not a fan of every story or all of the artwork, but since Triple Feature is a series of issues and not a stand-alone piece, I have absolutely no problem reading these tales while I wait for the next installment of the main arc.