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Here are the Highlights from Rihanna's Savage X Fenty Fashion Show during #NYFW
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Rihanna's Savage X Fenty fashion show during the New York Fashion Week is definitely one fashion show that has got social media buzzing. The show took place on Tuesday night (September 10) at the Barclays Center in Brooklyn, N.Y.
There was so much to unpack from the show; from the different celebrities who walked the red carpet to major music performances, a star-studded runway show and some head-turning carnival-themed headpieces.
While attendees weren't allowed to have phones or cameras out (so no one was able to capture content to post online), we've got a few of the photos for you! The show itself will be broadcast on Amazon Prime in a few days.
Rihanna is gorgeous in an Alexandre Vauthier dress on the red carpet.
See the highlights below.
BROOKLYN, NEW YORK – SEPTEMBER 10: Rihanna attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Slick Woods attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Halima Aden attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Normani attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Chika attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: G-Eazy attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Diplo attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Shanina Shaik attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Halsey attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Sabrina Dhowre Elba attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Wale (L) attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Saweetie attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: <> attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Ashley Graham attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Kehlani attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Paris Hilton attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Vanessa Hudgens attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Tierra Whack attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Naturi Naughton attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Nicky Hilton Rothschild attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Diane von Fürstenberg (L) and Talita von Fürstenberg attend Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Patrick Schwarzenegger attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Big Sean attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Mohammed Al Turki attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Jayla Koriyan attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Kitty Cash attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Toni Garrn attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Chanel Iman attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Saint Jhn attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Renell Medrano (L) and A$AP Ferg attend Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Dascha Polanco attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Loey Lane attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: (L-R) Quavo, Offset, and Takeoff of Migos attend Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Fat Joe attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: DJ Khaled attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Cara Delevigne attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Bella Hadid attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Kevin Mazur/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Gigi Hadid attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
BROOKLYN, NEW YORK – SEPTEMBER 10: Joan Smalls attends Savage X Fenty Show Presented By Amazon Prime Video – Arrivals at Barclays Center on September 10, 2019 in Brooklyn, New York. (Photo by Dimitrios Kambouris/Getty Images for Savage X Fenty Show Presented by Amazon Prime Video )
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text:
News Corp. promotes James Murdoch
By Sue Chang
SueChang
Markets reporter
SAN FRANCISCO (MarketWatch) -- News Corp. NWS, +0.73% said Wednesday it named James Murdoch deputy chief operating officer, and appointed him as chairman and chief executive of its international operations. Among other duties, Murdoch will develop and execute strategies that strengthen and further evolve businesses, brands, and new franchises, News Corp. said. He will also continue to maintain direct responsibility for the company's operations in Europe and Asia. Murdoch will relocate to New York, continue to report to Deputy Chairman, President and COO Chase Carey and work closely with Chairman and CEO Rupert Murdoch.
News Corp Cl B U.S.: Nasdaq: NWS

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AstraZeneca vaccine use can continue, pending blood clot probe -EMA
European countries can keep using AstraZeneca's coronavirus vaccine during an investigation into cases of blood clots that prompted Denmark, Norway and Iceland to suspend jabs, the EU's drug regulator said on Thursday.
There had been 30 cases of 'thromboembolic events' among five million people who've had the jab so far in Europe, the Amsterdam-based European Medicines Agency (EMA) said in a statement.
"The position of EMA's safety committee… is that the vaccine's benefits continue to outweigh its risks and the vaccine can continue to be administered while investigation of cases of thromboembolic events is ongoing," the EMA said.
"There is currently no indication that vaccination has caused these conditions, which are not listed as side effects with this vaccine."
Denmark, Norway and Iceland on Thursday temporarily suspended the use of AstraZeneca's Covid-19 vaccine over concerns about patients developing post-jab blood clots.
The EMA said Denmark's decision was a "precautionary measure while a full investigation is ongoing into reports of blood clots in people who received the vaccine, including one case in Denmark where a person died".
Of the 30 blood-clot cases across Europe, it said that "the number of thromboembolic events in vaccinated people is no higher than the number seen in the general population".
The EMA covers the 27-nation EU plus Norway, Iceland and Lichtenstein.
Italy's medicine regulator said Thursday it was banning a batch of the AstraZeneca/Oxford coronavirus vaccine over the issue.
Austria announced it had suspended the use of a different AstraZeneca batch, after a 49-year-old nurse died of severe blood coagulation days after receiving the shot.
Estonia, Latvia, Lithuania and Luxembourg have also suspended the use of the same batch as Austria.
AstraZeneca vaccine
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Norwich's Darren Webster through to last eight of PDC World Championships
Chris Wise
Published: 2:07 PM December 28, 2017 Updated: 3:04 PM October 10, 2020
Darren Webster celebrates after cruising past Toni Alcinas on day 12 of the William Hill World Darts Championship. Picture: PA - Credit: PA
Norwich's Darren Webster moved smoothly into the last eight of PDC William Hill World Championship after thrashing outsider Tony Alcinas 4-0 at the Alexandra Palace.
The 23rd seed went into the match against a man ranked outside the world's 100 as hot favourite to progress and made his class tell in a one-sided encounter.
Webster was only ever seriously troubled in the third set, when he had to come back from two legs down to prevail, and quickly wrapped the match up after that minor scare to set up a last eight clash against either Jamie Lewis, who beat James Richardson 4-1.
'It doesn't matter who you play you've got to go up there and play the board,' said Webster. 'I'm really pleased with my performance, I'm chuffed with that.
'I've got no taller but I'm rolling back the years, what I lack in height I make up for in heart and passion.
'In the next round it's irrelevant who I'm playing. People are saying you're the only seed left but is that good or bad? All the seeds around me have dropped out so I can't think about that.
'I've got one mission and that's to get up there on that board and do my job.
'I'm just going to chill out and get ready for tomorrow for whoever, bring them on!'
Webster kicked off with a 15-darter to get the match under way and after Alcinas levelled he recorded a 148 checkout to go in front before clinching the set with a break.
A 14-darter did the damage in the second set, with a 72 finish grabbing another break before Webster took out 75 for the second set.
Alcinas finally found his range in set three to move 2-0 ahead but his 49-year-old opponent produced the perfect response by holding his throw, breaking back and then taking the decider to stretch his lead to 3-0. It was then a case of closing the match out and Webster duly won the fourth set 3-0 to book his place in the last eight for the second time, and the first since way back in 2007.
His win was built around his accuracy at the doubles, with 52 per cent of his chances being converted, while a solid average of 94.92, with three 180s, was more than enough to see off a man who had done well just to reach the last 16.


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Q: Common current limit resistor for multiple LEDs? First, I realize the "common resistor for multiple LEDs" question has been asked. However, I have a different case where the LEDS are FET driven and reverse logic.
I have the following circuit. The circuit is actually four more of what is shown, i.e. all 16 outputs are used. The selector chip outputs are sinking type. The current to the LEDs is controlled by an external voltage controlled current source.
Since I never plan to turn on more than one output at a time, I would like to know if I can use a single, common current limiting resistor for all the LEDs? In other words, all the anodes (pin2) of the LEDs would be connected together and R8 would feed them all.
I'm thinking it would be ok if ensure the following: Start with current source=0 and turn on 3.3V.  Set all selector outputs to ON, thus turning off all the FETs.  Apply the desired current using the external current source, then finally turn off the selector output for the FET I would like to turn on. Continuing I would turn off the first LED prior to turning on the next LED. Note that I will not be switching LEDs very fast at all, only once every few seconds.

A: Absolutely, this is perfectly fine. In fact, I'm doing the same thing in a project on my workbench right now.
If this was not good practice, you could not really use a LED matrix. There is no way to add a resistor to each individual LED:

As Arsenal points out in a comment, you don't even need a resistor, if you actually have a current source. Just set the current to whatever current you want through the LED. The resistor does absolutely nothing here except wasting heat. If you do this, however, I suggest that you turn on the transistor before turning on the current. Otherwise, the current source will try to push current somewhere, and hopefully hit a ceiling before it finds a way.

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\part{}

\section*[Supplementary Materials]{Supplementary Materials\\ Thermography of the superfluid transition in a strongly interacting Fermi gas}
\author{Zhenjie Yan}
\thanks{Present address: Department of Physics, University of California, Berkeley, California 94720.}
\affiliation{\affcua}
\author{Parth B. Patel}
\author{Biswaroop Mukherjee}
\affiliation{\affcua}
\author{Chris J. Vale}
\affiliation{Optical Science Centre and ARC Centre of Excellence in Future Low-Energy Electronics Technologies, Swinburne University of Technology, Melbourne 3122, Australia}
\author{Richard J. Fletcher}
\author{Martin Zwierlein}
\affiliation{\affcua}

\section{Materials and Methods}

A strongly interacting Fermi gas of $^6$Li atoms is initially prepared in an equal mixture of the first and third lowest hyperfine states, ${\ket{1} \equiv \ket{m_J = -\frac{1}{2}, m_I=1}}$ and ${\ket{3} \equiv \ket{-\frac{1}{2}, -1}}$, at a magnetic field of $B=690 \,\rm G$, the location of the broad Feshbach resonance between these two states~\cite{Zurn2013}. The box potential is formed by walls of 532 nm light~\cite{Mukherjee2017b} and has cylindrical symmetry with a radius of $60\,\mathrm{\mu m}$ and a length of $90\,\mathrm{\mu m}$.
The Fermi energy of the system is $E_F=10.5(3)\ h \cdot \mathrm{kHz}$ corresponding to a density of $n_0=0.75(3)\ \mathrm{\mu m ^{-3}}$  per spin state or a Fermi temperature of $T_\mathrm{F} \simeq 500\ \mathrm{nK}$.
Evaporation in the uniform trap leads to a temperature $T\lesssim 0.1\,T_\textrm{F}$.
An additional heating step via periodic modulation of the box potential is used to finely control the temperature of the cloud.
To excite temperature gradients and second sound in the gas, we either apply an oscillating potential gradient, or alternatively we imprint an intensity-modulated light grating (Fig.~\ref{fig:S1}).
The potential gradient is applied magnetically, by adding current on one of the magnetic field coils generating the Feshbach field. The amplitude of the magnetic field oscillation is less than 0.02 G, much less than the width of the Feshbach resonance ($\Delta B \approx 170\,\rm G$)~\cite{Zurn2013}, such that the modulation of atomic interactions is negligible.
The oscillating gradient potential can generate a standing wave of first or second sound in the $m=1$ spatial mode, when the oscillation frequency is resonant.
The intensity-modulated grating potential serves as a local heat source in the atomic cloud. For this we employ 589 nm laser light to project a light-intensity grating onto the atoms. The grating spacing on the atomic cloud is $7\ \mathrm{\mu m}$. The intensity modulation is set to a frequency of 2 kHz, where phonons are efficiently created and rapidly decay into heat.
The amplitude of the grating modulation is kept at a low level so that the change in density and excitation of first sound is negligible.

To detect the temperature change in the system, a 0.5 ms rf pulse with a Rabi frequency of $\Omega_\mathrm{R}=2\pi\cdot1.9\ \mathrm{kHz}$ is used to transfer atoms in state $\ket{1}$ to the second lowest hyperfine state $\ket{f}\equiv\ket{2}=\ket{m_J = -\frac{1}{2}, m_I=0}$.
For thermometry at gas temperatures below $T = 0.15 T_\textrm{F} \approx 0.9 T_c$, an rf detuning of $5$ kHz is used. For data obtained above $0.15\ T_\textrm{F}$, taken via the local heating method, a range of detunings from $2$ to $5$ kHz is used to improve temperature sensitivity.
The local densities $n_\mathrm{f}(\mathbf{r})$ and $n(\mathbf{r})$ of transferred atoms in state $\ket{f}$ and unaffected atoms in state $\ket{3}$ are imaged after the rf pulse.
The spatial resolution of rf thermometry is dominated by diffusion of the transferred $\ket{2}$ atoms through the background of $\ket{1}$-$\ket{3}$ atoms during the $0.5$ ms pulse time. The interaction between rf-transferred $\ket{2}$ atoms with atoms in states $\ket{1}$ and $\ket{3}$ is weakly repulsive with $k_F a_{23}=0.21$ and $k_F a_{12}=0.26$. The diffusivity of a $\ket{2}$ atom can be estimated with $D_{2i} \approx \frac{\hbar}{m}\frac{1}{(k_F a_{2i})^2}$, with $i\in \{1,2\}$, leading to a diffusion distance during the pulse time of about $10\,\rm \mu m$. This estimate agrees with direct measurements of this diffusion on a localized sample of $\ket{2}$ atoms, created in a $\ket{1}$-$\ket{3}$ background via localized Raman beams.

\begin{figure}[b]
\includegraphics[width=6.75in]{FigS1.pdf}
\centering
\caption{\textbf{Two methods for creating second sound and heat gradients} (\textbf{A}) Second sound created by an oscillating potential gradient. The expansivity of the gas allows exciting temperature gradients through potential gradients.
(\textbf{B}) Creating temperature gradients using an intensity modulated light grating applied to one side of the box-trapped gas. Rapid modulations (at $2\,\rm kHz$) create short-wavelength phonons that rapidly decay into heat. In both \textbf{A} and \textbf{B} the blue to red color gradient represents an induced temperature variation from cold to hot.
}
\label{fig:S1}
\end{figure}

\section{RF Thermometry}

\begin{figure*}
\includegraphics[width=6.75in]{FigS2.pdf}
\caption{\textbf{Calibration of the temperature dependence of the rf transfer at constant density $\frac{\partial{n_f}}{\partial T}\Bigr|_n$.} (\textbf{A}) Rf transfer fraction $n_f/n_0$ at various temperatures and detunings in the superfluid phase. In the regime below $T/T_\textrm{F} = 0.15$, we find a maximum linear gradient along the temperature axis at a detuning of $5\,\rm kHz$, marked by the gray vertical line.
(\textbf{B}) The temperature dependence of the rf transfer rate across the superfluid transition (vertical dotted line). The green (yellow) circles are the measured rf transfer fraction at a detuning of 5 kHz (2 kHz).
The dashed lines are hyperbolas used to fit the rf transfer rate.
}
\label{fig:S2}
\end{figure*}

The sensitivity to temperature of the rf transfer is all that is needed to obtain a response from second sound and heat diffusion. The response would not need to be calibrated just to measure the speed and damping of second sound. However, by calibrating the response of the rf transfer to temperature, $\frac{\partial{n_f}}{\partial T}\Bigr|_n$ (rf-temperature response) and to density, $\frac{\partial{n_f}}{\partial n}\Bigr|_T$ (rf-density response), we can directly obtain the density-density and the density-temperature response functions of the unitary Fermi gas.
We calibrate the rf transfer at various temperatures and rf detunings, working at constant atom density (Fig.~\ref{fig:S2}A). For temperatures between $\sim 0.08$ and $0.15\,T_\textrm{F}$, a detuning of $\omega=2\pi \cdot 5\ \mathrm{kHz}$ is optimal, for which the temperature dependence of the transferred fraction $n_f/n_0$ is almost linear in temperature (Fig.~\ref{fig:S2}B).
Above the transition temperature, the rf transfer at $5\ \mathrm{kHz}$ detuning saturates with increasing temperature. Therefore, when working close to and above $T_c$, we employ a smaller detuning, as in the measurement of the thermal evolution after local heating.
A hyperbola is used to fit the rf-temperature responses and extract the local slope.
To calibrate the response of the rf transfer to density at constant temperature, we adiabatically ramp up a linear gradient potential along the axial $z$-direction and measure the change in both $n(z)$ and $n_\mathrm{f}(z)$, as shown in Fig.~\ref{fig:S3}A. The potential ramp is slow enough so that the temperature stays constant across the cloud. The transferred atom number is seen to decrease with increasing initial density, as expected for a clock shift that increases with density.
A linear fit to the $n_\mathrm{f}(\Delta n)$ curve gives the rf-density response, as shown in Fig.~\ref{fig:S3}B. The temperature dependence of the rf-density response $\frac{\partial{n_f}}{\partial n}\Bigr|_T$ is shown in Fig.~\ref{fig:S3}C, displaying maximal sensitivity, about a quarter of the actual density variation, near $T/T_F = 0.14$.

\begin{figure*}[b]
\includegraphics[width=6.75in]{FigS3.pdf}
\caption{\textbf{Calibration of the density dependence of the rf transfer at constant temperature $\frac{\partial{n_f}}{\partial n}\Bigr|_T$.}
(\textbf{A}) Density change along the axial direction in the state $\ket{f}$ $\Delta n_\mathrm{f}(z)$ (black) and state $\ket{3}$ $\Delta n(z)$ (red) after an adiabatic gradient ramp and the rf pulse. %
Only the data measured away from the edges of the cloud (marked by the vertical dotted lines) are used for the calibration (solid line).
(\textbf{B}) The linear response of rf transfer rate to the density change (black circles). $\frac{\partial{n_f}}{\partial n}\Bigr|_T$ is determined by a linear fit (dashed line).
(\textbf{C}) $\frac{\partial{n_f}}{\partial n}\Bigr|_T$ measured at various temperatures below $T_c$.
}
\label{fig:S3}
\end{figure*}

Having calibrated the temperature and density dependence of the rf transfer, we obtain the local temperature change via the relation
\begin{equation}
\Delta T(\bold{r},t) = \frac{\partial T}{\partial n_\mathrm{f}}\Bigr|_n \left[\Delta n_\mathrm{f}(\bold{r},t) - \frac{\partial n_\mathrm{f}}{\partial n}\Bigr|_T \Delta n(\bold{r},t)\right].
\label{Temperautre}
\end{equation}
Our measurements capture another crucial thermodynamic quantity that is the change in the reduced temperature $\tilde{T}=T/T_\textrm{F}$, given by the relation
\begin{equation}
\Delta \widetilde{T} (\bold{r},t)=\frac{\Delta T(\bold{r},t)}{T_\mathrm{F}}-\frac{2T}{3T_\mathrm{F} }\frac{\Delta n(\bold{r},t)}{n_0}.
\label{NormalizedT}
\end{equation}
In our scale invariant, unitary Fermi gas, the reduced temperature dictates the state of the system~\cite{Ho2004}. The entropy per particle $s = k_B f(\tilde{T})$ is a direct function of $\tilde{T}$, and the change $\Delta \tilde{T}$ directly yields the change in entropy via $\Delta s=c_V \Delta \tilde{T} / \tilde{T}$, since the specific heat $c_V = T\left.\partial s/\partial T\right|_n = k_B \tilde{T} f'(\tilde{T})$.
A measurement of the system's response in $\tilde{T}$ therefore directly yields the change in its entropy per particle, in units of the specific heat $c_V$.
Fig.~\ref{fig:S4} presents the individual responses of the density, rf transfer, temperature and reduced temperature after continuous oscillation of the potential gradient.
The density responds predominantly at the first sound resonance, with a faint response at the second sound resonance (Fig.~\ref{fig:S4}A). The rf transfer instead predominantly responds at the second sound resonance (Fig.~\ref{fig:S4}B).
Converting to absolute temperature changes $\Delta T$, we see that similar to the density response the strongest feature is from first sound. However, the response in reduced temperature $\Delta(T/T_F)$, which directly measures entropy changes, is strongest for the second sound resonance.
We have thus directly shown that second sound is an {\it entropy} wave (rather than a temperature wave) in a unitary Fermi superfluid, while first sound is an essentially isentropic density wave.
It is also evident that the rf transfer is a close proxy of the local entropy change. This is intuitively clear in the simplified picture of Fig.~\ref{fig:M1}, where the rf transfer predominantly excites the gas of excitations, e.g. pair breaking excitations, which directly determine the entropy of the gas.

\begin{figure*}
\includegraphics[width=6.75in]{FigS4.pdf}
\caption{\textbf{Steady state response of density $\Delta n$ (A), rf transfer $\Delta n_\mathrm{f}$ (B), temperature $\Delta T$ (C), and reduced temperature $\Delta (T/T_\textrm{F})$ (D).} In a unitary Fermi gas, the reduced temperature corresponds to entropy per particle. The measurements shown here are done at a temperature of $T/T_\textrm{F}=0.125$.
}
\label{fig:S4}
\end{figure*}

\section{Testing hydrodynamic scaling of second sound damping}

The validity of hydrodynamics relies on local thermal relaxation being much faster than the frequency of a propagating disturbance. While damping rates of first and second sound are similar, second sound is much slower than first sound, and thus its frequency for a given spatial mode is much lower than that of the corresponding first sound. The criterion for full two-fluid hydrodynamicity is therefore much more stringent for heat transport than for density (mass) transport. The breakdown of hydrodynamics affects the expression for the sound damping rate $\Gamma$. While $\Gamma \propto k^2$ in the hydrodynamic regime, so that $\Gamma/k^2$ can be interpreted as a diffusivity, the damping rate rather scales linearly with $k$ in the collisionless regime. The crossover was experimentally observed in ~\cite{Patel2020} for first sound to occur at frequencies $\omega \lesssim 0.2\, mc_1^2 /\hbar$ at temperatures below $T_c$, where $c_1$ is the speed of first sound. For our system, for first sound, only the eight lowest box modes ($m\lesssim 8$) are safely in the hydrodynamic regime. For second sound, therefore, we should expect only the lowest two spatial modes ($m\lesssim2$) to display hydrodynamic scaling of their damping rates.

To test hydrodynamic scaling, we were able to directly measure the frequency and damping rate of second sound in the $m=2$ mode. To excite this mode we imprint a potential using a 1064 nm laser beam focused at the center of the cloud, with a beam waist of $\sim 30\mathrm{\mu m}$, about one third of the box length. The intensity of the beam is modulated at the resonant frequency of the $m=2$ second sound mode, setting up a standing wave of second sound in $m=2$. Fig.~\ref{fig:S5}A shows the subsequent free time evolution of the temperature profile $\Delta T(z,t)$ after the end of the laser modulation. The corresponding Fourier amplitude $\Delta T(k_2,t)$ at $k_2=2\pi/L$ is shown in Fig.~\ref{fig:S5}B. As it should be for linear dispersion, the frequency of the $m=2$ is twice as high as for the corresponding $m=1$ mode (compare to Fig.~\ref{fig:M2}), i.e. the obtained speed of second sound is identical. The damping rate $\Gamma$ is found to be four times as high for $m=2$ than for $m=1$, as expected for hydrodynamic scaling. Fig.~\ref{fig:S5}C and D present the $m=2$ data points for speed and diffusivity together with the results for $m=1$. This consistency confirms that the observed damping rate $\Gamma$ for second sound is in the hydrodynamic regime for $m=1$ and $m=2$ and allows to uniquely define a second sound diffusivity $D_2= \Gamma/k^2$.

\begin{figure*}[!ht]
\includegraphics[width=6.75in]{FigS5.pdf}
\caption{\textbf{Testing hydrodynamic scaling with the $\mathbf{m=2}$ spatial mode of second sound.} (\textbf{A}) Axial temperature profile $\Delta T(z,t)$ versus time after excitation of the second spatial mode $m=2$ supported by the box. (\textbf{B}) Fourier amplitude of the $m=2$ spatial mode of the temperature profile, $\Delta T(k_2,t)$ (blue circles). The dashed line is a fit with Eq.~\ref{eq:evolution}. The speed (\textbf{C}) and diffusivity (\textbf{D}) obtained from the evolution of the $m=2$ mode (red circle) is compared with the values measured for the $m=1$ sloshing mode (black circles), demonstrating linear dispersion of second sound and hydrodynamic scaling of damping rates.
}
\label{fig:S5}
\end{figure*}

\section{Response functions}
The complete linear hydrodynamics of the two-fluid model of superfluids can be described via response functions as shown by Hohenberg and Martin~\cite{Hohenberg1965a}.
The measured changes in density $\Delta n$, entropy $\Delta s$ and reduced temperature $\Delta (T/T_\textrm{F})$ under a periodically modulated potential drive $U$ are associated with the density-density response function $\chi_{n,n}(\mathbf{k},\omega)$, the entropy-density response function $\chi_{s,n}(\mathbf{k},\omega)$, and the $\widetilde{T}$-density response function $\chi_{\tilde{T},n}(\mathbf{k},\omega)$:
\begin{align}
{\Delta} n (\mathbf{k},\omega) =& - \mathrm{Im}\chi_{n,n}(\mathbf{k},\omega)\cdot U(\mathbf{k},\omega),
\label{res:E1A}\\
{\Delta} s (\mathbf{k},\omega) =& - {\mathrm{Im}\chi_{s,n}(\mathbf{k},\omega)} \cdot U(\mathbf{k},\omega), \label{res:E1B}\\
{\Delta} \widetilde{T} (\mathbf{k},\omega) =& - \mathrm{Im}\chi_{\tilde{T},n}(\mathbf{k},\omega)\cdot U(\mathbf{k},\omega) \label{res:E1C}
\end{align}
Since we measure the state of the system right after an integer number of modulation cycles, the relations only involve the imaginary part of the response functions, the out-of-phase response.
For a unitary Fermi gas, $\chi_{s,n}(\mathbf{k},\omega)$ and $\chi_{\tilde{T},n}(\mathbf{k},\omega)$ are simply related to each other via
\begin{equation}
    \chi_{\widetilde{T},n}(\mathbf{k},\omega)=\frac{\widetilde{T}}{c_V}\chi_{s,n}(\mathbf{k},\omega)
    \label{res:E1D}
\end{equation}
A spatial Fourier transform of the measured density or rf transfer responses is used to quantify the amplitude of density or reduced temperature changes at a certain wavenumber $k$:
\begin{equation}
{\Delta} n (k) = \frac{2}{L} \int_0^L \mathrm{d}z\ \Delta n(z) \cos(k z).
\label{Fourier}
\end{equation}
A linear gradient potential with slope $g$ only has a strong spatial Fourier component at the first fundamental mode of the box: $U(k_1=\pi/L)={4 g L}/{\pi^2}$. Hence, we mainly focus on the first Fourier mode of the responses in this work.

The general form of the density-density, entropy-density, and $\tilde{T}$-density response functions are~\cite{Hohenberg1965a}:
\begin{eqnarray}
\chi_{n,n}(\mathbf{k},\omega) &=& \frac{n_0 k^2}{m} \frac{-\omega^2+\gamma c_{20}^2 k^2-i \Gamma_{n,n} k^2\omega}{(\omega^2-{c_1}^2k^2+i D_1 k^2 \omega)(\omega^2-{c_2}^2k^2+i D_2 k^2 \omega)},
\label{res:E2A}\\
\chi_{s,n}(\mathbf{k},\omega) &=& k^2 \frac{-\alpha_p {c_{10}}^2{c_{20}}^2 k^2+i \Gamma_{s,n} k^2\omega}{(\omega^2-{c_1}^2k^2+i D_1 k^2 \omega)(\omega^2-{c_2}^2k^2+i D_2 k^2 \omega)},
\label{res:E2B}\\
\chi_{\widetilde{T},n}(\mathbf{k},\omega) &=& \frac{k_B T}{c_V E_F} k^2 \frac{-\alpha_p {c_{10}}^2{c_{20}}^2 k^2+i \Gamma_{s,n} k^2\omega}{(\omega^2-{c_1}^2k^2+i D_1 k^2 \omega)(\omega^2-{c_2}^2k^2+i D_2 k^2 \omega)}.
\label{res:E2C}
\end{eqnarray}
Here, $\gamma=c_p/c_V$ is the isentropic expansion coefficient. $\gamma-1$ controls the relative weight of the second to the first sound peak in the density response.
$\alpha_p=\frac{1}{V}{\frac{\partial V}{\partial T}}\bigr|_p$ is the thermal expansivity, and it controls the strength of the second sound peak in the entropy-density response. $\alpha_p$ also represents the static susceptibility of the change of entropy to an applied potential $U$. Indeed, one has the Maxwell relation giving the change in entropy per particle upon a change in chemical potential ${\rm d}\mu = -{\rm d}U$:
$\left.\frac{\partial s}{\partial \mu}\right|_{T} = -\frac{1}{V}\left.\frac{\partial V}{\partial T}\right|_p = - \alpha_p$.
We note that at unitarity, $\alpha_p = \frac{3}{2}\frac{1}{T}(\gamma-1)$ is directly proportional to $\gamma-1$.

By fitting the measured density-density response with Eq.~\ref{res:E1A} and \ref{res:E2A}, we can directly obtain the isentropic expansion coefficient $\gamma$ (Fig.~\ref{fig:S6}A), while fitting the normalized temperature-density response ($\widetilde{T}$-$n$-response) with Eq.~\ref{res:E1C} and \ref{res:E2C} gives the value of $\frac{k_\textrm{B} T\alpha_p}{c_V}$ (Fig.~\ref{fig:S6}B). At unitarity, we have $c_V = \frac{3}{2} \frac{\alpha_p}{n \kappa_T}$, where $\kappa_T$ is the isothermal compressibility. Therefore, the normalized temperature-density response is governed by the compressibility of the gas: $\frac{k_\textrm{B} T\alpha_p}{c_V} = \frac{\kappa_T}{\kappa_0} \frac{T}{T_F}$, where $\kappa_0 = \frac{3}{2} \frac{1}{n E_F}$ is the compressibility of a non-interacting Fermi gas at zero temperature.
Figs.~\ref{fig:S6}A-B compare the measured strengths of the density and normalized temperature response to the previously measured equation of state~\cite{Ku2012}, finding good agreement within the error.

All response functions share the same denominator and poles.
The shared denominator is the determinant of the linear hydrodynamic equations, and the poles are located at
\begin{equation}
    \omega_{i,\pm}=\pm\sqrt{{c_{i}}^2k^2-({D_i} k^2/2)^2}-i{D_i} k^2/2,\ \ (i=1\ \text{or}\ 2).
\end{equation}
$c_{10}=\sqrt{(\partial p/ \partial{\rho})_s}$ and $c_{20}=\sqrt{\frac{s^2}{m}\frac{\rho_s}{\rho_n}\frac{\partial T}{\partial s}\bigr|_p}$ are the uncoupled speeds of first and second sound, and their values are given by the equation of state and for $c_2$ also the superfluid fraction. The two sound modes are coupled by the isentropic expansion factor $\gamma$:
\begin{eqnarray}
{c_1}^2+{c_2}^2&=&{c_{10}}^2+\gamma {c_{20}}^2, \\
{c_1}{c_2} &=& {c_{10}} {c_{20}}.
\label{res:E3}
\end{eqnarray}
The measured coupling between two sound modes is weak, owed to the large difference in speeds, so that coupled and uncoupled sound speeds are almost identical, as shown in Fig.~\ref{fig:S6}C.
The diffusivities of the two sound modes $D_1$ and $D_2$ are both linear combinations of thermal conductivity $\kappa$, shear viscosity $\eta$, and bulk viscosities $\zeta_3$ in the unitary Fermi gas~\cite{Khalatnikov1965,Hohenberg1965a}.
Introducing $D_\kappa = \frac{\kappa}{\rho c_P}$, $D_\eta = \frac{4}{3}\frac{\eta}{\rho}$ and $D_\zeta = \rho \zeta_3$, as well as $D_{20} = D_\kappa + \frac{\rho_s}{\rho_n}(D_\eta+D_\zeta)$, one has the relations
\begin{align}
    D_1 + D_2 = D_\eta + D_{20} + (\gamma-1)D_\kappa\\
    c_1^2 D_2 + c_2^2 D_1 = c_{10}^2 D_{20} + c_{20}^2 \gamma D_\eta (1-2a)
\end{align}
with $a = \frac{1}{\rho s}\left.\frac{\partial p}{\partial T}\right|_n = \sqrt{\frac{\rho_s}{\rho_n}\frac{c_{10}^2}{c_{20}^2}\frac{\gamma-1}{\gamma^2}}$. For the unitary gas, this simplifies to $a = \frac{2}{3}\frac{c_V}{s}$.
Solving for $D_1$ and $D_2$, one obtains
\begin{align}
    D_1 = &\frac{c_1^2 (\frac{\rho_s}{\rho_n} +1)-c_{10}^2  \frac{\rho_s}{\rho_n} +(2a-1) c_{20}^2 \gamma}{c_1^2-c_2^2} D_\eta+\frac{\gamma c_1^2 - c_{10}^2}{c_1^2-c_2^2} D_\kappa+\frac{ (c_1^2 - c_{10}^2) \frac{\rho_s}{\rho_n} }{c_1^2-c_2^2} D_\zeta, \label{res:D1} \\
    D_2 = &\frac{c_{10}^2  \frac{\rho_s}{\rho_n} -c_2^2 \frac{\rho_s}{\rho_n}-(2a-1) c_{20}^2 \gamma}{c_1^2-c_2^2} D_\eta+\frac{c_{10}^2-\gamma c_2^2}{c_1^2-c_2^2} D_\kappa + \frac{(c_{10}^2-c_2^2) \frac{\rho_s}{\rho_n} }{c_1^2-c_2^2} D_\zeta.\label{res:D2}
\end{align}
A measurement of $D_1$ and $D_2$ alone does not allow to obtain the three individual diffusivities $D_\eta$, $D_\kappa$ and $D_\zeta$. However, the terms
$\Gamma_{n,n}$ and $\Gamma_{s,n}$, which govern the asymmetry of the sound peaks in the imaginary part of the response functions, are also functions of $\kappa$, $\eta$, and $\zeta_3$:
\begin{align}
    \Gamma_{n,n} & =\gamma D_\kappa  + \frac{\rho_s}{\rho_n} (D_\eta+D_\zeta) , \label{res:Gamma_nn} \\
    \Gamma_{s,n} & = \left(\frac{\rho_s}{\rho_n}D_\eta  + a\gamma D_\kappa \right) \frac{s}{m}.\label{res:Gamma_sn}
\end{align}
We see that the response functions enable to determine all thermodynamic and linear transport parameters of the unitary Fermi gas. In practice, determination of $D_\eta$, $D_\kappa$ and $D_\zeta$ separately involves taking the difference of noisy experimental data, leading to significant errors. Direct measurements of these quantities, e.g. by measuring the damping of shear flow to determine $\eta$ alone are necessary.
The measured entropy and density responses below the superfluid critical temperature are shown in Fig.~\ref{fig:S7}, and the corresponding response functions $\chi_{n,T}$ and $\chi_{n,n}$ are represented in Fig.~\ref{fig:S8}.

\begin{figure*}
\includegraphics[width=6.75in]{FigS6.pdf}
\caption{\textbf{Thermodynamics from response functions.}
\textbf{(A)} The isentropic expansion coefficient $\gamma$, obtained from the measured density response (blue circles), compared to the value obtained from the previously measured equation of state~\cite{Ku2012} (gray circles).
\textbf{(B)} The amplitude of the normalized temperature response (blue circles), compared to the prediction $k_B T \alpha_p/c_V$ (gray circles) from the equation of state~\cite{Ku2012}.
\textbf{(C)} Coupled and uncoupled speeds of sound. The black circles (diamonds) and blue circles (diamonds) are the coupled (uncoupled) speeds of first and second sound, $c_1$ ($c_{10}$) and $c_2$ ($c_{20}$).
The vertical dashed line and shaded area indicates the phase transition temperature and its uncertainty, from~\cite{Ku2012}.
}
\label{fig:S6}
\end{figure*}

\section{Free evolution following an excitation}

The free evolution of density, temperature, entropy etc. can also be expressed with the help of the response functions, as demonstrated by Kadanoff and Martin in Ref.~\cite{Kadanoff1963}. The general form of the time evolution of any physical quantities $A$ is
\begin{equation}
{\Delta} A (\mathbf{k},t) = \int_{-\infty}^{+\infty} \sum_{i,\pm} \left[\frac{A_{i,\pm}}{z-\omega_{i,\pm}(\mathbf{k})}  e^{-i z t}\right] \mathrm{d}z.
\label{evolution_fourier}
\end{equation}
Here $\omega_{i,\pm}(\mathbf{k})$ are the poles of the response functions at a given wave vector $\mathbf{k}$. The $A_{i,\pm}$ are determined by the initial conditions and the residue of the response functions
\begin{equation}
    A_{i,\pm}=\sum_{j} \lim_{\omega \rightarrow \omega_{i,\pm}} \left [(\omega - \omega_{i,\pm})\frac{\mathrm{Im}\chi_{A,A_j}(\mathbf{k},\omega)}{\omega}  \right] \delta A_j(\mathbf{k},0),
\end{equation}
where $\delta A_j(\mathbf{k},0)$ is the initial deviation of physical observable $A_j$ from the equilibrium state and $\chi_{A,A_j}$ is the response function connecting $A$ and $A_j$.
Carrying out the inverse Fourier transform in Eq.~\ref{evolution_fourier}, one sees that the free evolution has the same form as a superposition of two damped harmonic oscillators with frequencies $c_1 k$ and $c_2 k$, and damping rates $D_1 k^2$ and $D_2 k^2$.
The general free-evolution solution of second sound and heat diffusion is:
\begin{eqnarray}
    {\Delta} A (\mathbf{k},t)=
    \begin{cases}
    A_0 e^{-{D_2} k^2 t/2}\cos{(\sqrt{{c_{2}}^2k^2-({D_2} k^2/2)^2} t + \phi)},& \text{if } c_{2}k>{D_2} k^2/2\\
    A_+ e^{-({D_2}k^2/2+\sqrt{({D_2}k^2/2)^2-{c_{2}}^2k^2})t}+A_- e^{-({D_2}k^2/2-\sqrt{({D_2}k^2/2)^2-{c_{2}}^2k^2})t},              & \text{if } 0<c_{2}k<{D_2} k^2/2\\
    A_0 e^{-{D_2} k^2 t}.             & \text{if } c_{2}k=0\\
    \end{cases}
    \label{eq:evolution}
\end{eqnarray}
The functions in Eq.~\ref{eq:evolution} are used to fit the thermal evolution data in Fig.~\ref{fig:M2}. A collection of measured free thermal evolution data is shown in Fig.~\ref{fig:S9}.

\begin{figure*}
\includegraphics[width=6.75in]{FigS7.pdf}
\caption{\textbf{Steady state entropy and denity response under continuous modulation of a potential gradient.} (\textbf{A} and \textbf{B}) The normalized temperature (A) and density (B) response amplitude is obtained at wavenumber $k_1=\pi/L$. An oscillation amplitude of $g=h \cdot 2.12 \ (0.85)\ \mathrm{Hz}/\mathrm{\mu m}$ and 5 (20) shaking cycles is used for oscillation frequencies below (above) 50 Hz. The solid lines are fits using Eq.~\ref{res:E2A} and \ref{res:E2C}.
}
\label{fig:S7}
\end{figure*}

\begin{figure*}
\includegraphics[width=6.75in]{FigS8.pdf}
\caption{\textbf{The normalized temperature-density response function $\mathrm{Im}\chi_{\tilde{T},n}(k_1,\omega) = \frac{\widetilde{T}}{c_V} \mathrm{Im}\chi_{s,n}(k_1,\omega)$, directly giving the entropy-density response (A) and the density-density response function $\mathrm{Im}\chi_{n,n}(k_1,\omega)$ (B).} The solid lines are fits to Eq.~\ref{res:E2A} and \ref{res:E2C}.
}
\label{fig:S8}
\end{figure*}

\begin{figure*}
\includegraphics[width=4in]{FigS9.pdf}
\caption{\textbf{Free evolution of temperature changes across the superfluid transition.} The thermal amplitude $\Delta T$ is obtained at wavenumber $k_1=\pi/L$. The dashed lines are fits with Eq.~\ref{eq:evolution}.
}
\label{fig:S9}
\end{figure*}

\section{Testing linear response of second sound}

Proper interpretation of the obtained response functions requires the second sound excitation to remain in the linear response regime. This is verified in two distinct ways. First, we fit the thermal evolution $\Delta T (k,t)$ with the solution of a damped harmonic oscillator (Eq.~\ref{eq:evolution}) in a time range $t\geq\tau_\mathrm{f}$. By varying $\tau_\mathrm{f}$, we effectively measure the frequency and decay rate of second sound at various initial amplitudes. We find the acquired frequency $\omega=c_2 k$ and damping rate $\Gamma=D_2 k^2$ to be independent of the fitting range. Secondly, we measure the amplitude of second sound excited by a resonant gradient oscillation and find a linear dependence on the oscillation amplitude $g$ (Fig.~\ref{fig:S10}A and B). The measured damping rate is also independent of the oscillation amplitude $g$ (Fig.~\ref{fig:S10}C).

\begin{figure*}[!ht]
\includegraphics[width=6.75in]{FigS10.pdf}
\caption{\textbf{Testing linear response.} (\textbf{A}) The amplitude of second sound generated by resonant excitation using an oscillating potential gradient of strength $g$. The dashed line is a linear fit to the data. (\textbf{B}) Ratio between the amplitude of second sound and gradient oscillation. The horizontal dashed line is the slope of the linear fit in (A). (\textbf{C}) The damping rate of second sound measured after resonant gradient oscillation. The horizontal dashed line is the width of the reduced temperature response $\Delta\frac{T}{T_\textrm{F}}(k_1,\omega)$ measured at $g=2.12\ h\cdot\mathrm{Hz/\mu{m}}$. The data shown here are measured at a temperature of $T/T_\mathrm{F}=0.12.$
}
\label{fig:S10}
\end{figure*}

\end{document}

redpajama_set_name: RedPajamaArXiv


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Lauri Knapton is the founder of Knapton Musik Knotes in Janesville, Wisconsin. The store, which was established in 2000, provides musical instruments, lessons, and a long list of community outreach programs such as Rock Camp and Uke Circles. Lauri has been passionate about music since she began...
Music Retail, Women in the Music Industry, Wisconsin, Music Lessons, Music Education, RPMDA, Lowrey Organs
Roger Kraft
Roger Kraft was a pioneer in the retailing of electronic musical instruments such as keyboards and synthesizers in the 1980s. Many may recall the days of keyboard stores throughout the United States in the early days of MIDI, when innovative keyboards were the craze. With a background in...
Music Retail, MIDI, Synthesizers, Wisconsin, Keyboards
John LaBouve
John LaBouve's background is in business and marketing. When he married into the Goodell Family, he took a chance at working in his father-in-law's music store, Goodell Music in Sheboygan, WI. He began in 1974 and soon took over the store as president and owner. During the interview, John discussed...
Music Retail, Wisconsin, Band and Orchestra, Guitars, Percussion, Drums


text:
Angels' October surprise: Season ends way too early as Royals sweep
Angels center fielder Mike Trout walks to the dugout as the Kansas City Royals celebrate their series-clinch victory in Game 3 of the ALDS on Sunday. (Robert Gauthier / Los Angeles Times)
Kansas City Royals players celebrate the team's series-clinching, 8-3 win over the Angels in Game 3 of the ALDS on Sunday. (Robert Gauthier / Los Angeles Times)
Angels center fielder Mike Trout watches his solo home run during the first inning of Game 3 of the American League division series against the Kansas City Royals on Sunday. (Robert Gauthier / Los Angeles Times)
Angels center fielder Mike Trout rounds the bases after hitting a solo home run during the first inning of Game 3 of the ALDS against the Kansas City Royals on Sunday. (Robert Gauthier / Los Angeles Times)
Angels starter C.J. Wilson delivers a pitch during the first inning of Game 3 of the American League division series against the Kansas City Royals. (Jamie Squire / Getty Images)
Kansas City Royals starter James Shields delivers a pitch against the Angels during the third inning of Game 3 of the American League division series on Sunday. (Robert Gauthier / Los Angeles Times)
Angels starter C.J. Wilson looks on after giving up a three-run triple to Kansas City's Alex Gordon (not pictured) during the first inning of Game 3 of the ALDS on Sunday. (Robert Gauthier / Los Angeles Times)
Angels starter C.J. Wilson is pulled from the game in the first inning after giving up a three-run triple in Game 3 of the ALDS against the Kansas City Royals. (Robert Gauthier / Los Angeles Times)
Kansas City Royals baserunner Billy Butler slides under the tag of Angels catcher Chris Iannetta to score during the first inning of Game 3 of the ALDS on Sunday. (Robert Gauthier / Los Angeles Times)
Kansas City's Eric Hosmer, left, celebrates with teammate Billy Butler after hitting a home run during the third inning of Game 3 of the ALDS against the Angels on Sunday. (Robert Gauthier / Los Angeles Times)
Angels first baseman Albert Pujols hits a solo home run during the fourth inning of the team's 8-3 loss to the Kansas City Royals in Game 3 of the ALDS on Sunday. (Robert Gauthier / Los Angeles Times)
Angels center fielder Mike Trout walks back to the dugout after striking out to seal the Kansas City Royals' 8-3 win in Game 3 of the ALDS on Sunday. (Robert Gauthier / Los Angeles Times)
Angels center fielder Mike Trout reacts during an at-bat against the Kansas City Royals in the third inning of Game 3 of the ALDS on Sunday. (Robert Gauthier / Los Angeles Times)
Kansas City Royals teammates Norichika Aoki, left, and Billy Butler celebrate after scoring in the first inning against the Angels in Game 3 of the American League division series on Sunday. (Jamie Squire / Getty Images)
Kansas City Royals pitcher James Shields reacts after striking out an Angels batter during the sixth inning of the team's 8-3 win in Game 3 of the ALDS on Sunday. (Robert Gauthier / Los Angeles Times)
Kansas City Royals outfielder Lorenzo Cain makes a diving catch during the fifth inning of an 8-3 win over the Angels in Game 3 of the ALDS on Sunday.
(Robert Gauthier, Los Angeles Times)
Angels starter C.J. Wilson delivers a pitch during the first inning of Game 3 of the ALDS against the Kansas City Royals on Sunday. (Robert Gauthier / Los Angeles Times)
Angels players talk to pitcher Hector Santiago, right, during the third inning of Game 3 of the ALDS against the Kansas City Royals on Sunday. (Robert Gauthier / Los Angeles Times)
Angels players leave the dugout after the team's season-ending loss to the Kansas City Royals in Game 3 of the ALDS on Sunday. (Robert Gauthier / Los Angeles Times)
Angels starting pitcher Jered Weaver is one of the last players to leave the dugout following the team's season-ending loss to the Kansas City Royals in Game 3 of the ALDS on Sunday. (Robert Gauthier / Los Angeles Times)
By Mike DiGiovannaStaff Writer
Reporting from Kansas City, Mo. —
General Manager Jerry Dipoto was convinced the Angels could win not only Sunday night's do-or-die game against the Kansas City Royals "but 10 more games" if they could get their high-powered offense on track.
"This team can be electric when we get it rolling," Dipoto said. "Really, it's just tipping the rock off the cliff and letting it go."
But that rock turned out to be a boulder, the cliff was a steep incline, and the Angels were Sisyphus. Every push was met with Royal resistance; every inch of ground they gained, they'd lose a yard until they were ultimately crushed by a Royal force they could not slow.
Kansas City completed a three-game American League division series sweep of the Angels with an 8-3 Game 3 victory before a rowdy, broom-wielding crowd of 40,657 in Kauffman Stadium, where it poured Angels relievers, actual rain at times and eventually champagne, which flowed freely in the home clubhouse.
The Royals' first playoff appearance since 1985 will continue in the AL Championship Series against the Baltimore Orioles starting Friday.
The Angels' first playoff appearance since 2009 ended abruptly, with three straight losses, a bitter finish to a season in which they forged a major league-best 98-64 record and seemed primed for a deep October run.
"It's not the way we wanted it to end, but give the Royals a lot of credit," said Angels center fielder Mike Trout, who struck out to end the game. "When they needed a big play, they made it. When they needed a big hit, they got it. Offensively, we didn't do our jobs. It's tough."
After losing a pair of 11-inning games in Anaheim, Trout gave the Angels their first lead of the series with his first playoff hit, a home run to left field off Royals starter James Shields in the first inning.
But Alex Gordon roped a three-run double off C.J. Wilson in the bottom of the first, ending the Angels starter's night after two-thirds of an inning, and Eric Hosmer hit a two-run homer in the third for a 5-1 Kansas City lead.
Albert Pujols led off the fourth with a homer to make it 5-2. Erick Aybar doubled with one out, his second of four hits, and David Freese was hit by a pitch. But Josh Hamilton grounded into a fielder's choice, C.J. Cron struck out to end the inning, and Kansas city tacked on two in the bottom of the fourth for a 7-2 lead.
Then with two on in the fifth, Royals center fielder Lorenzo Cain robbed Pujols and Howie Kendrick of hits, racing to shallow left-center for a diving catch of Pujols' liner and to shallow center for a sliding catch of Kendrick's flare, Cain's teammates doffing their caps to him in reverence.
"If my ball drops, maybe Trout eventually scores from first, and instead of 7-2 it's 7-4, and anything can happen," Pujols said. "But they made some great plays. It seems like the momentum never went our way."
Blame the enigmatic and erratic Wilson for that. In the biggest start of his Angels career, the veteran left-hander came up Lilliputian, failing to get out of the first inning and yielding to a parade of seven relievers.
Manager Mike Scioscia made it clear before the game that Wilson would be on a short leash, saying, "Our whole staff is going to have to get it done if one guy stubs his toe." Wilson didn't stub his toe. He tripped over himself and fell down a flight of stairs.
Nori Aoki and Cain singled with one out in the first. The next two plate appearances captured Wilson in a nutshell — he struck out Hosmer on three pitches and walked Billy Butler on four pitches to load the bases.
Gordon drove a curve on the outside corner to the wall in left-center to give the Royals a 3-1 lead, and Scioscia pulled Wilson, making his the shortest non-injury-related playoff start since St. Louis left-hander Rick Ankiel lasted two-thirds of an inning against the New York Mets on Oct. 12, 2000.
"I felt like I was physically, mentally and strategically prepared, I just didn't execute that last pitch," Wilson said. "I had a good plan. I tried to get him to hit a fly ball to Trout, and he hit it harder than I thought.
"You make one bad pitch in a game like this, and that's it. It's a little surreal. I feel like it puts an exclamation point on the fact that I couldn't get anything to go my way."
And a period to the Angels' season.
Mike DiGiovanna
Mike DiGiovanna is a sports writer who contributes to the coverage of the Dodgers, Angels and Chargers for the Los Angeles Times.


text:
In October 1997, Kevin Barnes launched String Theory, a unique radio show which explores a world of compelling music, on 88.5 FM.
Join as at The Dakota, Sunday, November 12th from 4 to 6 p.m. for a special celebration featuring performances by a wonderfully diverse group of String Theory friends including: Dean Magraw, Steven Hobert, Congolese guitarist Siama Matazungidi and Dallas Johnson, Tim Sparks, Robert Everest, Brian Barnes and Diane Jarvi , and Patrick O'Loughlin and Tim Reese.
Tickets are $20 with a portion of proceeds benefiting Jazz88.
Catherine Russell is featured for the evening show at 7 p.m.
http://kbem-recast.streamguys1.com/content/u20171110080307143.mp3
Kevin Barnes talks with Emily Reese about String Theory's 20th anniversary celebration on the Morning Show, Nov. 10, 2017.
Jennifer Eckes, Arne Fogel perform in White Bear Lake


text:
BetFury es una empresa internacional de apuestas de i-gaming. El proyecto fue lanzado en 2019.

Antecedentes
BetFury es una marca de i-gaming y juegos de azar que se lanzó en 2019. Destaca por introducir la criptomoneda en la plataforma de juegos de azar online que permite a los jugadores apostar jugando a diferentes juegos en la plataforma y recompensarlos con Bitcoin.

Según su página web, los jugadores pueden jugar desde posiciones remotas en todo el mundo a través de canales seguros. El sistema de pago está encriptado para proteger todo el sistema de transacciones. En los últimos tiempos, la empresa ha pasado de Tron a Bitcoin como su principal fuente de transacciones. Una de las características de BetFury es su sistema de Dividendos, que permite la obtención de gotas multidivisa para todos los poseedores de BFG. El valor del token BFG puede incrementarse invitando a nuevos jugadores a minar.

Licencia
BetFury es una plataforma de juego con licencia. La empresa posee la licencia de juego Universe B Games B.V., lo que la convierte en una empresa de confianza limitada. Está registrada bajo el gobierno de Curazao con una licencia auténtica en Curazao. El número de registro de la licencia de Curazao es 155126. Otras licencias son proporcionadas por Gaming Services License Providers N.V, proporcionando a BetFury el derecho a un "Casino BTC" y a operar más allá de las fronteras geográficas.

Referencias

Criptomonedas
Cadenas de bloques
Casas de apuestas digitales

redpajama_set_name: RedPajamaWikipedia


Charming Kitchen Design Ideas On A Budget #16 - Small Bathroom Vanities For Small Bathroom was uploaded in July 19, 2018 at 1:34 am. If you wish to use this picture as your desktop wallpaper, you can tap the download link beneath or you may just right click on the photo above , then pick "Save Image As" to download the Charming Kitchen Design Ideas On A Budget #16 - Small Bathroom Vanities For Small Bathroom or by choose the "Set Desktop Background As" choice if your internet browser has this option. If you could not obtain the the best image you are hoping for, you need to go for "Search Column" at top right or browse some other picture backgrounds whichever you wish. This picture has the image size is 92kB and the dimension of 910x986. Charming Kitchen Design Ideas On A Budget #16 - Small Bathroom Vanities For Small Bathroom has been seen by 16 viewers and it is an attachment from Kitchen Design Ideas On A Budget.


What's in the February 12th Update?
We know many of you are patiently waiting for the new updates we promised a few weeks back, but due to some issues while testing, we had to reschedule the update for February 12th. However, despite all the setbacks we've had during development, we are confident of the February 12th release, and is positive you will absolutely enjoy the new upcoming features trakdesk has to offer.
Here is a short list of features and fixes that will be included in the February 12th update.
Ability to copy and paste images into the text editor when replying to tickets and creating knowledgebase articles.
CSV export in specific user locale.
Read-time browser notifications when tickets are created and responded to.
Real-time ticket updates notification beacon when tickets are updated by agents. Live notifications also works with macros, time-based and event-based automations.
Inline ticket message reply. Completely removed ticket popup reply.
Thanks for the information regarding the update. We really appreciate your dedication to improving Trakdesk.
Some really great new features…TrakDesk is getting better and better with each update youd…excellent support system.


text:
Диетическое питание () — регламентированное употребление пищи для уменьшения, поддержания или увеличения массы тела, а также для предотвращения и лечения таких заболеваний, как диабет и ожирение. Диета для похудения рекомендуется людям с проблемами со здоровьем, связанными с лишним весом, но не здоровым людям. Поскольку потеря веса зависит от количества потребляемых калорий, было показано, что различные виды низкокалорийных диет (с низким содержанием жиров, с низким содержанием углеводов и т. д.) не более эффективны, чем другие. После прекращения курса диеты вес обычно восстанавливается частично или полностью, поэтому эффективность той или иной диеты следует оценивать в долгосрочном периоде. Кроме того, результаты диетического питания могут широко варьироваться в зависимости от человека.

По статистике, почти половина взрослых американцев когда-либо пыталась похудеть с помощью диеты.

История

Слово диета происходит от греческого diaita, означающего не только узкую схему похудания, но здоровый образа жизни в целом, включая как психическое, так и физическое здоровье.

Одним из первых диетологов был английский врач Джордж Чейни. Имея избыточный вес , Чейни перешёл на постную диету, употребляя только молоко и овощи, и вскоре выздоровел. Он начал публично рекомендовать свою диету всем, кто страдает ожирением. В 1724 году Чейни написал эссе «Очерк здоровья и долгой жизни» (An Essay of Health and Long Life), в котором советовал заниматься физическими упражнениями на свежем воздухе и питаться, избегая калорийных деликатесов.

В 1797 году шотландский военный хирург  опубликовал «Записки о диабете» (Notes of a Diabetic Case), где описал преимущества мясной диеты для страдающих сахарным диабетом. Он первым применил открытие гликозурии, сделанное английским врачом , к диагностике диабета и лечению нарушений обмена веществ. Ролло разработал диету, которая оказалась успешной при лечении диабета 2 типа.

Первым популяризатором низкоуглеводной диеты был не диетолог или врач, а королевский плотник-гробовщик Уильям Бантинг . В 19 веке он написал и издал в 1868 году небольшой буклет под названием «Письмо о тучности, адресованное общественности» ( англ. Letter on Corpulence, Addressed to the Public), который стал одной из самых известных из когда-либо написанных книг об ожирении, был много раз переиздан и продолжал публиковаться долгое время после смерти автора. В нём содержалось описание диеты, которой следовал он сам. Диета Бантинга состояла из четырёх приёмов пищи в день, включавших мясо, зелень, фрукты и сухое вино. Акцент делался на отказе от сахара, сладких продуктов, крахмала, пива, молока и масла. Брошюра Бантинга пользовалась популярностью долгие годы и использовалась в качестве модели для множества современных диет. Спустя почти 150 лет диета Бантинга была подтверждена несколькими клиническими испытаниями как безопасная и эффективная для похудания, а теперь она признана полезной диетой для людей, страдающих диабетом. Бантинг советовал переходить на диету только после «полной консультации с врачом».

Первой книгой о снижении веса на основе учёта калорийности продуктов стала книга 1918 года американского врача  «Диета и здоровье: влияние калорий» (Diet and Health: With Key to the Calories).

Подсчитано, что до 2014 года было разработано более 1000 диет для похудания.

Типы диет

Ограничительных диет чаще придерживаются желающие похудеть. Иногда диета соблюдается для того, чтобы набрать мышечную массу. Диеты также можно использовать для поддержания стабильной массы тела и улучшения здоровья. Различают следующие типы диет:
 Безжировая
 Безуглеводная
 Низкокалорийная
 Голодание
 Детокс
 Экологическая

Эффективность
Некоторые диеты позволяют избавиться от ожирения и добиться похудания, при этом успех диеты в большей степени зависит не от вида диеты, а от соблюдения режима питания. Метаанализ шести рандомизированных испытаний не выявил разницы между низкокалорийной, низкоуглеводной и низкожирной диетами, при потере веса на 2-4 кг за 12-18 месяцев во всех исследованиях. В некоторых случаях экстремальные диеты могут привести к болезненному исхуданию.

Основной проблемой снижения веса является необходимость строгого соблюдения диеты. Диета может эффективно способствовать снижению веса на короткое время, однако в долгосрочной перспективе трудно поддерживать достигнутое. Кроме того, недоедание подавляет термогенез скелетных мышц. Подавленный термогенез ускоряет набор веса после прекращения диеты, если только эта фаза не сопровождается физическими упражнениями (см. ).

Эффективность диеты индивидуальна, поэтому «средняя потеря веса» не является надёжным всеобщим показателем эффективности той или иной диеты. Метаанализ 29 американских исследований 2001 года показал, что участники программ похудания через пять лет сохраняли потерю, в среднем, 23 % от первоначальной потери веса. Устойчивое снижение массы тела в среднем составляло 3,2 %.

Ограничение питания, по-видимому, более эффективно для похудения, чем физические упражнения, но сочетание того и другого даёт ещё более долгосрочные результаты.

Побочные эффекты
 Повышенная смертность
Ряд исследований показал, что преднамеренная потеря веса связана с увеличением смертности у людей без проблем со здоровьем, связанных с весом.

 Пищевые добавки
Из-за экстремального или несбалансированного питания могут потребоваться пищевые добавки, обеспечивающие организм витаминами, минералами или другими веществами, которых может не хватать при несбалансированной диете. Несмотря на пользу для поддержания здорового образа жизни с несбалансированной диетой, добавками не следует злоупотреблять. Передозировка любой пищевой добавки может вызвать ряд побочных эффектов в зависимости от того, какая добавка была принята.

 Расстройства питания
Специалисты отмечают, что, при наличии определенных факторов риска, соблюдение диеты может привести к развитию расстройства пищевого поведения. Исследования показали, что диета и нездоровое поведение, связанное с контролем веса, в дальнейшем могут привести к ожирению и расстройству пищевого поведения. Специалисты рекомендуют «отказаться от диеты и радикальных мер контроля веса в пользу здорового питания и физических упражнений».

Методы питания
 Время приема пищи
График приема пищи, как известно, является важным фактором любой диеты. Недавние данные свидетельствуют о том, что новые стратегии планирования, такие как периодическое голодание или пропуск приема пищи, а также стратегически размещенные перекусы перед едой, могут быть рекомендованы для снижения сердечно-сосудистых рисков.

 Дневник
Исследование 2008 года, опубликованное в «Американском журнале профилактической медицины», показало, что те из сидящих на диете, которые вели дневник питания (или журнал диеты), теряли в два раза больше веса. Предполагается, что ведущие записи лучше осведомлены о том, что они потребляют, и поэтому потребляют меньше калорий.

 Вода

Наблюдения показали, что поощрение потребления воды и отказ от т. н. «энергетических напитков» облегчает снижение веса. Показано, что выпивание 500 мл воды перед едой в течение 12 недель привело к более длительному снижению веса.

Общество
Подсчитано, что в любой момент времени примерно 1 из 3 взрослых американцев соблюдает какую-либо диету. 85 % людей, сидящих на диете, составляют женщины. Расходы жителей США на диетические продукты и абонементы в тренажерные залы составляют около 60 млрд долл. ежегодно. 80 % людей, сидящих на диете, делают это самостоятельно и лишь 20 % обращаются к специалистам или присоединяются к платной программе. Типичный человек, сидящий на диете, делает 4 попытки в год.

 Группы похудания
Некоторые группы по снижению веса работают на коммерческой основе, другие — как благотворительные организации. К первым относятся  и
. Ко вторым — ,  и группы, созданные местными энтузиастами.

Методы этих организаций значительно различаются. Некоторые группы построены по программе , другие действуют по призвольным программам. Некоторые группы выступают за определенные готовые продукты или специальные меню, в то время как другие учат людей, сидящих на диете, делать выбор в пользу здоровой пищи как в ресторанах, так и при закупке продуктов и приготовлении пищи.
 Социальные стереотипы
Среди молодых женщин из высших слоев стран Запада распространено мнение, что упитаность и пышные формы есть признак дурного тона, что зачастую приводит к ограничению калорийности питания. Такое поведение может представлять серьезную опасность для здоровья.

См. также
 Образ тела
 Суперпища

Примечания

Литература

 Dansinger, M. L., Gleason, J. L., Griffith, J. L., et al., «One Year Effectiveness of the Atkins, Ornish, Weight Watchers, and Zone Diets in Decreasing Body Weight and Heart Disease Risk», Presented at the American Heart Association Scientific Sessions, Orlando, Florida, 12 November 2003.
 Schwartz, Hillel. Never Satisfied: A Cultural History of Diets, Fantasies, and Fat. New York: Free Press/Macmillan, 1986.

Ожирение
Диеты
Питание человека


text:
Pardon me?
by May 24th, 1996 August 29th, 2020
In keeping with his campaign promise to help D.C.'s "offender" community, Mayor Marion Barry has asked the D.C. Council to pass a bill that would empower him to grant clemency to people who break District laws. At first glance, the bill would transform Barry into Gerald Ford, allowing him to pardon a long line of friends, wives, and associates convicted of criminal offenses. But according to a council staffer, as currently written the bill would only allow the mayor to pardon petty criminals prosecuted by the D.C. Corporation Counsel, not the more serious criminals prosecuted by the U.S. Attorney. So rather than pardon, say, mayoral assistant and convicted murderer Rhozier "Roach" Brown, Barry would be limited to liberating folks like "Carwash," the homeless guy who occasionally pees on the side of D.C. Superior Court. At-Large Councilmember Bill Lightfoot has invited Barry to testify at a June 19 hearing on the bill. No word yet on whether the mayor will attend.
Bogus Lotus In 1979, when Diane Hendel took up Transcendental Meditation (TM) under the paid tutelage of the D.C.-based World Plan Executive Council, the group promised her she would learn to fly, levitate, become invisible, and walk through walls. Today, Hendel cannot fly, nor can she levitate, become invisible, or walk through walls—and her knees are shot from too much time in the lotus position. As a result, Hendel wants her money back. But after seven years of litigation against the council and its founder, the Maharishi Mahesh Yogi, Hendel is still a long way from seeing green. D.C. Superior Court Judge Arthur Burnett ruled earlier this year that Hendel could not sue the group for fraud and unfair trade practices because TM is a religion, and the suit would involve the court in "excessive entanglement in religious beliefs." Still, a Chicago-based watchdog outfit, the Cult Awareness Network (CAN), has investigated the council's marketing claims, and several other alleged victims have squeezed big bucks out of the TM organization. Hendel is now appealing Burnett's decision with pro bono help from one of D.C.'s biggest law firms, Arent, Fox, Kintner, Plotkin & Kahn. Firm partner David Bardin says, "I don't think anybody considers meditation as such a cult activity. But there have been many people who have complained about this group."
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Free-Range Tofu Last Sunday, animal rights activists affiliated with United Poultry Concerns (UPC) swarmed around brunchers dining on the patio of the Belmont Kitchen in Adams Morgan. Staging its Sixth Annual Spring Mourning Vigil for Chickens, UPC used graphic posters of hundreds of hens crammed into battery cages and close-up shots of gruesome chicken tumors to make its point. UPC President Karen Davis, who runs a chicken sanctuary in Maryland, says that during egg production hens suffer painful debeaking, starvation, and severe electrocution. She hopes the protests will encourage people to "take an interest in the lives of chickens and understand them more compassionately." But Belmont Kitchen owner Jane Anderson was none too thrilled that the UPC protesters, who rode in from tony Potomac, Md., chose to stage their demonstration at her storefront during peak business hours. "I know chickens are abused, but we can't change 100 years of agricultural production by protesting in front of a community restaurant," says Anderson. "We have had tofu on our menu a couple of times and we had to throw it all out. We give people what they want."


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Emma Couceiro (Cospeito, Lugo, 1977) es una poeta española en lengua gallega.

Biografía
Es licenciada en Filología hispánica por la Universidad de La Coruña, tiene publicado los poemarios Humidosas (V Premio Espiral Maior de Poesía, Espiral Maior, 1997), As entrañas horas (X Premio Eusebio Lorenzo Baleirón, Ediciós do Castro, 1998) e (Cito) (Xerais, 2003). Colaboró como poeta en revistas como A Xanela, Dorna, Xistral ou Zurgai y en los volúmenes colectivos Mulher a fazer vento, Palabras no ar ou Novas voces da poesía galega y Recital, entre otros.

Rasgos estílisticos
Su poética se caracteriza por una indagación cotidiana en el yo lírico, muchas veces articulada a través de la técnica del desdoblamiento As entrañas horas, por el uso de símbolos y repeticiones (Humidosas), y por el empleo de una sintaxis rota y ambientación íntima que nos remite muchas veces al territorio del hogar (marcado en menino) y al marco de la infancia.
Es considerada por la crítica gallega como una de las voces más interesantes de la llamada "Generación de los 90".

Obras

 Humidosas. Espiral Maior, 1997.
 As entrañas horas. Edicios do Castro, 1998.
 Cito. Xerais, 2003.

Galardones

V Premio Espiral Maior de Poesía.
X Premio Eusebio Lorenzo Baleirón.

Enlaces externos
Emma Couceiro en Galicia, mujeres poetas (II)

Biografía en BVG
Emma Couceiro en Antología de Joven Poesía Galega

Alumnado de la Universidad de La Coruña
Couceiro, Emma
Couceiro, Emma


text:
Q: new MongoId objects with php I am trying to create new objects on MongoDB via PHP with personalized IDs, like this:
    $user = Array(
        '_id'  => "$id",
        'name' => $name,
    );

The problem with this is that when I query for IDs, I need to use the following:
$query = Array( '_id' => "$id" );

instead of the more appropriate
$query = Array( '_id' => new MongoId("$id") );

forcing me to change all the queries. I thought that I do it by fixing the inserting, by putting '_id'  => new MongoId("$id") but, if I use that, it will simply create the default
mongodb id, insead of my personalized one.
How can I fix this?
Thanks in advance

A: I am a little confused by exactly what you are asking for here, however, I believe I might just understand.
If you are using a _id different to the default ObjectId that MongoDB uses for the primary key of a row then you should not use ObjectId or in fact MongoId to create that object.
You should only use MongoId when you using the default _id that is provided, if you use your own the ObjectId (MongoId) will not function as you expect.
So the answer here is to stop using the MongoId.


Most girls have a fetish for varied collection of shoes. Thus, whenever there is a special event or party, women crave for some of the best shoes. No matter, whether you are attending a special party or it is your regular day at office, appropriate shoes are definitely essential.
Most girls have a fetish for varied collection of shoes. Thus, whenever there is a special event or party, women crave for some of the best shoes. No matter, whether you are attending a special party or it is your regular day at office, appropriate shoes are definitely essential. So, it is definitely essential to understand the features of various ladies footwear such that your hard earned money is rightly spent. Though the basic criteria of shoes is definitely comfort but these days fashionable designs and patterns also play a crucial role. Thus, you should always select perfect shoes for every occasion.
Online shoe shopping comes as a great option as it allows shoppers to make a selection at their own pace. If you want to buy shoes for your office use, leather shoes definitely works best. Again, for party wear you can pick from a wide range of heels. No matter what designs you choose, it is always better t look for the comfort. In fact, for price you should never compromise on the level of comfort. Once you wear comfortable shoes you will realize that it is definitely worth your money. If you want to understand the features of the shoes, you can easily have a look at the online stores. So, this summer go for online shoe shopping and buy exceptional ladies footwear.
The major benefit of online shoe shopping is that is offers plenty of opportunity to save a huge amount of money. Moreover, you also get an unlimited range of options to choose from. Thus, shopping becomes easier and simple. In fact, at online stores you also get products from reputed brands. Thus, quality is something which you can always be assured off. Once it gets delivered, it is always essential that you check the fittings of the shoes. If by any chance you pick the wrong shoes, online stores also gives you the opportunity to return it in a hassle free manner. So, go for online shoe shopping and buy exceptional ladies footwear. You can also select brands like aldo shoes and other products.
If you try purchasing aldo shoes at physical stores, it may charge a high amount of price. On the other hand you can easily get these selected Aldo shoes at lesser rates if you choose to shop online. So, stop wasting your money in wrong pair of shoes , rather buy exceptional ladies footwear by online shoe shopping.
Avni Mehra is a famous writer for online shopping in India. She has written many articles on India shopping, online shoe shopping, aldo shoes, ladies footwear and many more in India.


text:
package com.gambit.sdk.pubsub.exceptions;

/**
 * Thrown when a  socket implementation is unusuable. The exception is not
 * differentiated from whether it exists or is unusuable for some other reason.
 */
public class PubSubSocketImplementationException extends PubSubException
{
    /**
     * Creates this PubSubSocketImplementationException with the given message.
     *
     * @param message Message to associate with this PubSubSocketImplementationException.
     */
    public PubSubSocketImplementationException(String message) {
        super(message);
    }
}

redpajama_set_name: RedPajamaGithub


One of my more savvy Gold Coast hotel clients recently contracted me last week for a very quick photo shoot. They needed promotional photos of one of their entertainment areas that they book for corporate and private events.
The space was a very nice one, very sellable, yet they had no photos of it to promote the hotel's offering with.
Just a super-quick shoot while the space was already dressed for an event was proposed to increase their bookings. A tiny fraction of what they charge for one event booking was all that it took to invest in some nice photography to immediately multiply their ROI.
Good images of your venue are vital – be it a restaurant, cafe, hotel or event space for hire. Prospective clients need to see images that clearly represent the offering if they are to consider short-listing your venue for their event.
Another tip is to photograph your venue at both day and night times, if your event hours offer both timing options. Don't rely on people's ability to visualise your venue at night through daytime interior/exterior photos. You'll be missing the opportunity to showcase the magic of your venue once the mood lighting and candles are in place for an event.
For enquiries regarding hotel, restaurant, cafe or event photography, please do contact us for further advice about how to best fulfil your specific needs.


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Jonathan Hung: "I Am Hopeful We Can Soon Be Home To Space Unicorns, Not Just Start-Ups"
5 Best Spa Staycations To Kick Off 2021
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Dr Caroline Low-Heah, Ken Khoo, Jessie Ho-Thong and Michelle Lim Hope To Do Plenty Of Good This Holiday Season
Retrospective 2020: Tan Min Lan, Antoinette Patterson, Dennis Ye, Teodor Andius, Weiman Kow & Sim Bee Hia
Shirley Crystal Chua's Golden Equator Is Committed To Propelling Possibilities
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Has Filmmaker Loretta Chen Found The Secret To Happiness In Bhutan?
She talks about her latest film and what it means to be an artist in Singapore. Spoiler: it isn't easy.
Take Note
The Agenda: Preludio's New Menu, Makeup Releases From Charlotte Tilbury, And Other Things You Need To Know
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The world doesn't just consist of them, but Hollywood certainly acts like it does.
The Agenda: Where To Countdown The New Year, Party-Ready Jewellery From Louis Vuitton, And Other Things You Need To Know
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The Cultural And Political Sway Of Red
Beyond being a festive signifier, the colour red has always carried cultural significance. Here are some of the memorable parts it has played throughout history.
The Agenda: New Jewellery From Dior, Chantecaille's Holiday Collection, And Other Things You Need To Know
The Agenda: A New Van Cleef & Arpels Bracelet, Etro's Holiday Collection, And Other Things You Need To Know
All Hail The Fan!
No mere culture vultures, fans today are actively demonstrating their devotion to movies, music and TV shows in ways that are shaking up the pop cultural landscape. Here's a journey through fandom that proves it's not about what you love, but how you love it.
The Agenda: A Pop-up Wine And Dine Event, Christie's Watches And Jewellery Auction, And Other Things You Need To Know
The Agenda: Genderless Perfumes From Atelier Versace, Zenith's New Chronomaster 2, And Other Things You Need To Know
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Your go-to list of the best things to shop, see and experience.
A Magazine Singapore is a print and online luxury lifestyle title published by Apical Media. Singapore is our home base, but our lively mix of editorials stretches far and wide. Like our audience, we have an affinity for the good life — fashion, watches & jewellery, art & culture, travel, food & wine; we are also mindful and empowered, and want in on the important conversations, from global trends to social issues.
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HomeHomeWhy Interest rate futures market is struggling to pick up in India?
Interest rate futures (IRFs) were first introduced as a concept in 2003 but it took another 6 years before it actually took off in 2009. The idea of interest rate futures is to hedge your interest rate risk which is the possible price loss caused by a rise in interest rates. However, this is one market segment that has not really taken off in India in a big way. For example, the currency derivatives that were introduced at the same time have seen very strong traction on the NSE and the BSE and commodities have also picked up. However, IRFs have left a lot to be desired. Let us first look at the concept of IRFs and its advantages before getting into why it has not taken off in India.
What are IRFs all about?
An Interest Rate Future is an agreement to buy or sell a debt instrument at a future date for a price fixed today. When you buy or sell an IRF, you buy or sell the bond in terms of a price fixed and not in terms of yields. You basically use the reverse approach; you buy the IRFs for a fall in interest rates and you sell the IRFs for an anticipated rise in interest rates. The underlying security for IRFs is usually a government bond or a treasury bill. Currently, the RBI has permitted trading of IRFs in Treasury Bills and in long dated 10-year benchmark bonds. Remember that IRFs have dual regulation by the RBI and SEBI. While RBI focuses on the interest rate impact of IRF trading, SEBI is more concerned about the securities market trading issues pertaining to IRFs.
What are IRFs used for?
Interest Rate Futures are primarily used to hedge or offset interest rate risks. Interest rate risk is the risk you are exposed to when you have an interest payable or receivable. If you are holding a fixed rate bond, then increase in rates becomes a risk because the bond prices will fall. When you are holding floating rate bonds, then fall in rates will mean lower yields and that becomes a risk for you. Basically, when you hedge, you take position in the futures market that is the opposite of that in the cash market. Like in most hedging activities, IRF has a cost in terms of hedging cost and the opportunity cost. The value of the contract goes up and comes down as market interest rates rise and fall.
Here is how an individual can practically use IRFs. If you have a floating rate home loan and expect the interest rate to go up in the coming 3 months it will mean that your borrowing cost will go up and so will your EMI. Are you prepared for that? You can offset this interest rate risk by selling interest rate futures contract. So if interest rates go up, the price of the contract for you falls and you make profits on the short IRFs. You can buy it back at a lower price and make profits. The advantage the IRFs enjoy vis-à-vis equity derivatives is that there is no securities transaction tax (STT). This makes it a lot more efficient.
Why have IRFs not taken off in India?
IRFs are still work in progress. There are a few reasons why they are yet to take off.
Interest rate risk is still not so well understood risk in India as equity price risk, default risk and volatility risk. Most traders and investors still equate government bonds with absolute safety and hence don't understand the concept of hedging their interest rate risk.
The concept of hedging loan risks with IRFs is yet to take off in a big way in India. That is where the potential lies and that is what needs to be marketed as a business solution to the customers.
Retail holding in government securities is still too limited and hence the need for retail investors to hedge risk is not seen today. That has limited the participation in this market substantially.
Bond pricing in India is still not too efficient due to a restricted bond market and controlled interest rates. Till this issue is resolved and the yield curve develops, IRFs may face challenges for now!
What are the benefits of IRFs?
Interest Rate Futures are primarily used to hedge or offset interest rate risks. Interest rate risk is the risk you are exposed to when you have an interest payable loan or have invested in interest earning instrument.
How are interest rates futures priced?
I hold an account with Tradeplus, can I trade in IRFs?
You can trade in interest rate futures if you have activated currency segment for you.