text:
Odile Decq (Studio Odile Decq)
Fangshan Tangshan National Geopark
Odile Decq first came to prominence in 1990 with the completion of Banque Populaire de L'Ouest in Rennes, designed with her late husband and partner Benoît Cornette. In recent years, she has completed the extension to the Museum of Contemporary Art in Rome (2010), The Phantom Restaurant at the Opéra Garnier in Paris (2011), FRAC Bretagne Contemporary Art Museum in Rennes (2012), the renovation of Antti Lovag's bubble house Maison Bernard in France (2016) and Le Cargo office space for tech start-ups in Paris (2016). In 2016, she was awarded the Jane Drew prize for women in architecture.
In this talk, Decq discusses her Fangshan Tangshan National Geopark Museum in Nanjing China (2014). Inspired by the way bondage accentuates the curves of the female body, she designed a building that responds to and exaggerates the existing landscape with a central atrium that varies floor to floor to challenge the prescriptive circulation of traditional museums.
Decq also spoke to us about setting up her influential Confluence Institute (see The Confluence Institute: Rethinking Architectural Education), which offers a radical alternative to conventional architectural education.
Recorded at Studio Odile Decq in Paris, France. August 2017.
Odile Decq
Odile Decq The Confluence Institute: Rethinking Architectural Education 2017
Julia Barfield Rethinking The Classroom: University Of Cambridge Primary School 2017
Dominique Perrault Ewha Womans University: Building As Landscape 2017
James Timberlake The New London Embassy: An Expression Of American Power 2018


text:
No Alcohol Or Drugs Involved in Death of Robin Williams
Oscar-winning actor and comedian Robin Williams did not have alcohol or illicit drugs in his system, according to the final autopsy report.
Wife: Robin Williams Had Parkinson's, Was Sober When He Died
Nov. 7, 2014, 9:20 PM UTC / Updated Nov. 7, 2014, 11:52 PM UTC
Comedian and actor Robin Williams did not have alcohol or illicit drugs in his system when he committed suicide on Aug. 11, the final autopsy report released Friday by the Marin County Sheriff's Office shows. But Williams was suffering from depression, anxiety, the early stages of Parkinson's Disease and increasing feelings of compulsion and paranoia, the report states.
Williams, 63, died of "asphyxia due to hanging," at his home in Tiburon, California, as the preliminary autopsy report revealed. The Oscar-winning legend battled addiction for decades but had been sober for many years.
He was diagnosed with Parkinson's in 2013, two years after he developed symptoms, such as a left arm tremor and slowing of his left hand's movements. He was taking medication in "therapeutic concentrations" which improved his condition and kept him physically active until his death, the report says.
According to the report, Williams and his wife, Susan Schneider, had been sleeping in separate bedrooms because he was having trouble sleeping. He "would sometimes move around a lot in bed or talk loudly in his sleep," according to the report.
In late June, Williams checked into a retreat facility in Minnesota but "he did not check in for drug or alcohol abuse," his wife told investigators. It had been suggested to Williams that he use the retreat to rejuvenate the principles of his 12-step program and apply them to "facets of his life he was having trouble with," the report states.
The night before Williams died, he had been concerned about a watch collection and put several of them in a sock and drove them to an unidentified person's house, the report states. That behavior exemplified the feeling of paranoia his wife felt was escalating, the report states. But Williams never spoke of suicidal thoughts. Analysis of his iPhone, iPad and laptop revealed no suicide-related searches on the Internet, the report states.
When his wife awoke on Aug. 11, she assumed Williams was sleeping and she went out to run errands. Williams' assistant found his body a few hours later, after becoming concerned for his well-being and breaking into the bedroom. Williams was fully dressed in jeans and a black T-shirt, the report states.
The day after the comedy legend died, he was cremated and his ashes were scattered over the San Francisco Bay, his death certificate states.
Robin Williams' Ashes Scattered Over San Francisco Bay
Robin Williams Suffering From Early Parkinson's, Wife Says
Robin Williams Dead at 63

redpajama_set_name: RedPajamaCommonCrawl


study or even run a business. A common misconception is that a couple must be married in order to apply for a spousal visa – but in reality, it is a visa which is ideal for married couples or even permanent life partners of two years or more.
If unmarried, it is important to have a notarial contract which attests to the fact the relationship has been one of good faith for a period of at least two years – and is monogamous in nature. It is equally as important to illustrate proof of shared finances in the form of shared bank accounts, home insurance, lease agreements, etcetera.
Since the case of Stewart and Others v Minister of Home Affairs and Others, it is now possible for an applicant who is in South Africa on a tourist visa in terms of section 11(1) to change the condition of their visa to a spousal visa from within the country.


text:
\section{Introduction}

Although Einstein's theory of general relativity (GR) is well-established, it is unlikely to be completed at ultra-violet energy scales on its own. This is because, in a similar manner to Fermi's effective theory for weak interactions, Newton's constant characterizing the strength of the gravitational coupling carries units of length-squared. The formation of black holes at Planck scale energy density and the concurrence  of space-time singularities further obscure the nature of gravity at short distances, where quantum effects becomes important.

To unify gravity and quantum mechanics, string theory predicts that GR should be augmented with new degrees of freedom in such a way that supersymmetry is respected at sufficiently high energy scales. In perturbative string theory, quantum corrections to GR can in principle be calculated at each string loop order, in which taking the low energy limit yields an infinite series expanded in powers of the string length squared $\ell_s^2$, with supersymmetry preserved order by order in $\ell_s^2$. Four-dimensional supergravity models preserving eight supercharges arise as low energy limits of string theory compactified on Calabi--Yau 3-folds. The leading higher-derivative corrections to the Einstein--Hilbert action contain terms quadratic in the curvature tensor coupled to scalar fields.

The recent observations of gravitational waves (GW) from binary black holes \cite{GW150914} and neutron stars \cite{GW170817} mergers have extended the success of GR from the low-velocity, weak gravitational field regime to a highly dynamical regime governed by strong gravity. Interestingly, effects from string-inspired Einstein--dilaton--Gauss--Bonnet and dynamical Chern--Simons gravity on gravitational wave emission have been seriously considered in exploring modifications to GR, as they result in the emission of scalar dipole (at 1PN) and quadrupole (at 2PN) radiation during the inspiral \cite{Nair:2019iur}. This could potentially revive interest in higher-derivative extended gravity models with a string theory origin with the advantage that, given a compactification scheme, the lower dimension couplings are fixed, thus increasing verifiability of the model.

   This paper is devoted to understanding exact solutions in higher-derivative extended supergravity models, which are notoriously hard.  Supersymmetric higher-derivative terms can be most conveniently organized using the off-shell formulation of supersymmetry, which is possible up to six dimensions ($D=6$), in which we set up the calculation. By consistent dimensional reduction, six-dimensional solutions give rise to solutions in lower-dimensional models. This leaves out a separate case in $D=5$ (and of course its reduction to lower dimensions) due to the possibility of introducing two inequivalent off-shell formulations \cite{Bergshoeff:2001hc}, which we leave for a future study. The main advantage of working in $D=6$ is that there are fewer fields, and so correspondingly the supersymmetry transformation rules are reasonably simple. For on-shell two-derivative supergravities in $D = 6$, there are classifications of supersymmetric solutions in \cite{GMR, CC, Cano:2018wnq, LV}. In this paper the approach uses the crucial fact that the off-shell supersymmetry transformation rules are theory-independent. Therefore, solutions to off-shell Killing spinor equations are universal to all theories invariant under the same supersymmetry transformations. One can thus use the known explicit supersymmetric solutions of the simplest two-derivative theory as a guide to deduce the structure of the off-shell Killing spinor applicable to other solutions with the same isometries. Substituting the ansatz for bosonic fields based on symmetry considerations and
   the universal form of the off-shell Killing spinor into the off-shell Killing spinor equations results in
   theory-independent algebraic relations amongst the undetermined functions. Therefore,
   without using equations of motion, we have partially solved the system for all supergravity models. Of course, fully determining the solutions requires dynamical input from a specific theory. For simplicity, we
   choose the $p$-form field equations as the dynamical input, which usually admit a first integral implied by the gauge symmetry. We elaborate this idea by constructing the supersymmetric, rotating, dyonic string solution in $D=6$ ungauged minimal supergravity coupled to a tensor multiplet with higher-derivative extensions. The static and rotating dyonic strings solutions in $D=6$ two-derivative supergravity were presented in  \cite{Duff:1993ye,DFKR,DKL,CL}.

   The near-horizon limit of the dyonic string solution leads to the conformally flat AdS$_3\times$S$^3$ vacuum preserving eight chiral supercharges. The central charges present in the asymptotic symmetry algebra of AdS$_3$ receive higher-derivative corrections. When the supergravity model arises from string theory, the AdS$_3$ vacuum admits a dual 2D conformal field theory (CFT) description. Comparing the higher-derivative corrected gravitational central charges to the CFT central charges then provides a precision test of the AdS$_3$/CFT$_2$ correspondence beyond the large central charge limit. Using our solution, we compute the higher derivative corrections to the Brown--Henneaux central charges in a particular model resulting from compactifying type IIA string theory on a K3 manifold.

\section{Rotating dyonic string solutions}

\subsection{Supergravity}

We begin by introducing the $D=6$ off-shell formulation of supergravity. The minimal supergravity multiplet combines with a self-dual tensor multiplet to form the off-shell irreducible dilaton--Weyl multiplet consisting of bosonic fields $\{g_{\mu\nu}\,,B_{\mu\nu}\,,L\,,V_{\mu}\,,V^{ij}_\mu\,,E_\mu\}$ and fermionic fields $\{\psi^i_\mu\,,\varphi^i\} $, with $i=1,2$ and $\mu$ labeling the 6D coordinate index. $\{V_{\mu}\,,V^{ij}_\mu\,,E_\mu\}$ are the auxiliary fields required by the off-shell closure of the supersymmetry algebra. The Einstein--Hilbert Lagrangian invariant under the 6D off-shell supersymmetry is given by
 \begin{equation}
\label{EHSUGRA}
{\cal L}_{\rm EH}=\sqrt{-g}\left(LR +L^{-1}\nabla^\mu L \, \nabla_\mu L - \ft{1}{12}L H^{\mu \nu \rho} H_{\mu \nu \rho}+\ldots\right)\,,\quad H_{\mu\nu\rho}=3\partial_{[\mu} B_{\nu\rho]}\,,
\end{equation}
where here and below the omitted terms are quadratic in auxiliary fields. This Lagrangian is written in string frame, which simplifies the supersymmetrization of higher-derivative terms. In addition to \eqref{EHSUGRA}, we add the recently constructed off-shell supersymmetric Gauss--Bonnet term \cite{NOPT}\footnote{Here we use the convention $\epsilon_{012345}=1$, so the $B\wedge R\wedge R$ term has a minus sign, whereas \cite{NOPT} has a plus sign. This sign difference results from a different convention for the chirality of fermions.}
\begin{eqnarray}
\label{GBSUGRA}
{\cal L}_{\rm GB} &=& \sqrt{-g} \left(  R_{\mu\nu\rho\sigma} R^{\mu\nu\rho\sigma} - 4 R_{\mu\nu} R^{\mu\nu} + R^2 + \ft16 R H^2 - R^{\mu\nu} H_{\mu\nu}^2 + \ft12 R_{\mu\nu\rho\sigma} H^{\mu\nu\lambda} H^{\rho\sigma}{}_{\lambda} \right. \nonumber \\
&& \left. + \ft{5}{24} H^4 + \ft{1}{144} (H^2)^2 - \ft18 (H_{\mu\nu}^2)^2 - \ft14 \epsilon^{\mu\nu\rho\sigma\lambda\tau} B_{\mu\nu} R_{\rho\sigma}{}^{\alpha}{}_{\beta} (\omega_+) R_{\lambda\tau}{}^{\beta}{}_{\alpha}(\omega_+)+\ldots \right)\,,
\end{eqnarray}
where $R_{\mu\nu\rho\sigma}$ is the standard Riemann tensor of $g_{\mu\nu}$, while $R_{\mu\nu}{}^{\alpha}{}_{\beta} (\omega_+)$ is the curvature associated with the torsionful spin connection $\omega_{+\mu}^{\alpha}{}_{\beta}$,
\begin{equation}
R_{\mu\nu}{}^{\alpha}{}_{\beta} (\omega_+)=\partial_{\mu}\omega_{+\nu}^{\alpha}{}_{\beta}+\omega_{+\mu}^{\alpha}{}_{\gamma}\,\omega_{+\nu}^{\gamma}{}_{\beta}-(\mu\leftrightarrow\nu)\,,\quad \omega_{+\mu}^\alpha{}_\beta=\omega_{\mu}^\alpha{}_\beta+\ft12H_{\mu}{}^\alpha{}_\beta\,.
\end{equation}
The shorthand notations for various contractions of $H_{\mu\nu\rho}$ are
\begin{equation}
H^2:=H_{\mu\nu\rho}H^{\mu\nu\rho}\,,\quad H_{\mu\nu}^2=H_{\mu\rho\sigma}H_{\nu}{}^{\rho\sigma}\,,\quad H^4:=H_{\mu\nu\sigma}H_{\rho\lambda}{}^{\sigma}H^{\mu\rho\delta}H^{\nu\lambda}{}_{\delta}\,.
\end{equation}
Other 6D off-shell supersymmetric higher-derivative actions can be found in \cite{BSS86}-\cite{BNOPT}. We prefer the Gauss--Bonnet combination to other higher-derivative invariants because it gives rise to relatively simple equations of motion while entailing enough complexity to display the efficiency of our method, especially when applied to non-static solutions.  Furthermore, going to Einstein frame, the model becomes the supersymmetric version of the Einstein--dilaton--Gauss--Bonnet gravity of broader interest. To summarize, in this section, we use the total action
\begin{equation}
S_{\rm EGB}=\frac1{16\pi G_6}\int d^6 x \left({\cal L}_{\rm EH}+\frac{1}{16}\lambda_{\rm GB}\,{\cal L}_{\rm GB}\right) ,
\end{equation}
where $G_6$ is the $D = 6$ Newton constant.  The action enjoys the scaling symmetry
\begin{equation}
(g_{\mu\nu}\,,B_{\mu\nu}\,,L\,,\lambda_{\rm GB}) \rightarrow (tg_{\mu\nu}\,,tB_{\mu\nu}\,,t^{-2}L\,,t^{-1}\lambda_{\rm GB} )
\label{scaling}
\end{equation}
needed in later discussions.

\subsection{Killing spinor equation}

The supersymmetric rotating string solutions can be derived from the 3-charge black string solution \cite{CL} by taking the limit in which the mass saturates the Bogomolny--Prasad--Sommerfield (BPS) bound set by the sum of all charges. Also, the two angular momenta are equal and the solution possesses an enhanced U(2) isometry \cite{GLPP}.
The explicit form of the solution is given by
\begin{eqnarray}
\label{CLs}
ds_6^2&=&\frac{r^2}{(r^2+Q)}\bigg[-\bigg( dt+\frac{J}{2r^2}\sigma_3 \bigg) ^2+ \bigg( dx+\frac{J}{2r^2}\sigma_3 \bigg) ^2 \bigg]
+(r^2+P)\frac{dr^2}{r^2}\nonumber \\
&&+\ft14(r^2+P)\left(\sigma_3^2+d\theta^2+\sin^2\theta d\phi^2\right)\,,\nonumber \\
B_{(2)}&=&2P\omega_2+\frac{r^2}{r^2+Q}dt\wedge dx+\frac{J}{2(r^2+Q)}dt\wedge\sigma_3+\frac{J}{2(r^2+Q)}\sigma_3\wedge dx\,,\nonumber \\
L&=&\frac{r^2+Q}{r^2+P}\,,
\end{eqnarray}
where $\sigma_3=d\chi-\cos\theta d\phi$, $d\omega_2=\textrm{Vol}(S^3)$, and the electromagnetic charges $Q$ and $P$ are positive. All auxiliary fields vanish for this solution. It is evident that the solution above is cohomogeneity-1 and admits a U(2)$\times\mathbb{R}^2$ isometry. The infinite string lies along the $x$-direction. When $r\to\infty$, the solution approaches Minkowski spacetime with energy and angular-momentum density along the string
\begin{equation}
{\cal M}=\frac{(Q+P)\pi}{4 G_6}\,,\qquad {\cal J}=-\frac{J\pi}{4 G_6}\,,
\end{equation}
where the angular momentum is associated with the Euler angle $\chi$. In the asymptotically flat case, the symmetry is given by the Poincar\'{e} superalgebra not involving the generators associated compact isometry of the solution. Therefore, the angular momentum does not enter the BPS bound. The supersymmetry of the solution \eqref{CLs} can be seen by explicitly solving the Killing spinor equations, which are given by the vanishing supersymmetry variations of the fermionic fields $\{\psi^i_\mu\,,\varphi^i\}$:
\begin{align}
\label{susyt}
& \bigg( \partial_{\mu} +\frac14\omega_{\mu
	\alpha\beta}\gamma^{\alpha\beta} \bigg) \epsilon^i-\frac12{V}_\mu\delta^{ij}\epsilon_j +{V}_\mu{}^i{}_j\epsilon^j +\frac18 H_{\mu\nu\rho}\gamma^{\nu\rho}\epsilon^i = 0 \, ,
\nonumber \\
& \frac{1}{2\sqrt 2} \gamma^\mu
\delta^{ij}\partial_\mu L \epsilon_j -\frac14 \gamma^\mu E_\mu\epsilon^i
+\frac{1}{\sqrt2}\gamma^\mu { V}{}_\mu^{(i}{}_k \delta^{j)k} L
\epsilon_j - \frac{1}{12\sqrt2}L\delta^{ij}\gamma_{\mu\nu\rho} H^{\mu\nu\rho} \epsilon_j = 0 \,,
\end{align}
where $\epsilon^i$ is a symplectic Majorana--Weyl spinor with the chirality  $\gamma_{012345}\epsilon^i=\epsilon^i$.  Indices $i, j, \ldots$ are raised and lowered by $\varepsilon^{ij}$ and $\varepsilon_{ij}$. For convenience, we introduce the
complex Weyl spinor
\begin{equation}
\epsilon=\epsilon_1+\textrm{i}\epsilon_2.
\end{equation}
Substituting \eqref{CLs} into \eqref{susyt}, we find the solution for $\epsilon$ given by
\begin{equation}
\label{ks1}
\epsilon=\frac{r^{1/2}}{(r^2+Q)^{1/4}}\epsilon_0\,,
\end{equation}
where $\epsilon_0$ is the Killing spinor on a two-sphere embedded in the $D=6$ spinor so that it satisfies the projection conditions
\begin{equation}
\gamma^{012345}\epsilon_0=-\epsilon_0\,,\quad \gamma^{01}\epsilon_0=-\epsilon_0\,.
\end{equation}
We now make an ansatz for supersymmetric rotating strings in generic supergravity models based on the same set of fields. The metric $g_{\mu\nu}$, two-form potential $B_{\mu\nu}$ and the scalar $L$ takes the form fixed by the U(2)$\times\mathbb{R}^2$ isometry
\begin{align}
\label{genstr}
ds_6^2&=a^2(r)\left[-(dt+\varpi\sigma_3)^2+(dx+\varpi\sigma_3)^2\right]
+b^2(r){dr^2}+\ft14c^2(r)\left(\sigma_3^2+d\theta^2+\sin^2\theta d\phi^2\right)\,,\nonumber \\
B_{(2)}&=2P\omega_2+d(r)dt\wedge dx+f(r)(dt - dx) \wedge\sigma_3 \,,\nonumber \\
L&=L(r)\,,
\end{align}
with vanishing auxiliary fields. The corresponding Killing spinor is assumed to be
\begin{equation}
\label{ks2}
\epsilon=\Pi(r)\epsilon_0\,,
\end{equation}
where $\epsilon_0$ is the same as in \eqref{ks1}. Substituting \eqref{genstr} and \eqref{ks2} into the Killing spinor equations \eqref{susyt} then yields the consistency relations
\begin{eqnarray}
\label{ks3}
&&\dot{d}-2 a \dot{a}=0\,,\quad \frac{\dot{d}}{a^2b}+\frac{\dot{L}}{Lb}-\frac{2 P}{c^3}=0\,, \quad \varpi \dot{d}-\dot{f}+a^2 \dot{\varpi}+\frac{2 f b}{c}-\frac{2 a^2b \varpi}{c}=0\,,\nonumber \\
&& \frac{P b}{c} -bc+c\dot{c}=0\,,\quad \Pi=\sqrt{a}\,,
\end{eqnarray}
where dots denote derivatives with respect to $r$. The conditions in \eqref{ks3} are necessary and sufficient conditions for the existence of Killing spinors corresponding to the rotating strings. The gauge symmetries in the system are related to the choice of coordinate $r$ and the Abelian one-form symmetry of $B_{(2)}$. We can fix the reparametrization of $r$ by demanding
\begin{equation}
c=rb\,,
\end{equation}
using which \eqref{ks3} can be readily integrated yielding
\begin{equation}
d=a^2+\kappa_1\,,\quad c^2=r^2+P\,,\quad \varpi d=f+\kappa_2 r^2\,,\quad L|d|=\frac{\kappa_3r^2}{r^2+P}\,.
\end{equation}
We then set $\kappa_1=0$ using the Abelian one-form symmetry and $\kappa_3=1$ using the scaling \eqref{scaling}. We consider the case in which the higher-derivative correction is small and the general solution obeys the same boundary condition as indicated by solution
\eqref{CLs}. Explicitly,
\begin{equation}
\label{bc}
a = {\cal O}(1)\,,\quad b = {\cal O}(1)\,,\quad c = {\cal O}(r)\,,\quad \varpi = {\cal O}(r^{-2})\,,\quad d = {\cal O}(1)\,,\quad f= {\cal O}(r^{-2})\,,
\end{equation}
which implies that $\kappa_2=0$. In summary, we have
\begin{equation}
\label{sol1}
a^2=d\,,\quad b^2=1+\frac{P}{r^2}\,,\quad c^2=r^2+P\,,\quad f=d\varpi\,,\quad L=\frac{r^2}{d(r^2+P)}\,,
\end{equation}
so have reduced the system to solving for two functions, $d(r)$ and $\varpi(r)$.  We emphasize that these relations are independent of the details of the Lagrangian, depending only on the set of fields in the model and the U(2)$\times \mathbb{R}^2$ symmetry of the solution.

The dynamical equations determining $d(r)$ and $\varpi(r)$, and therefore the whole system, come from the components of the $B_{(2)}$ field equation. The dilaton equation is automatically satisfied for the off-shell relations \eqref{sol1}. There are two independent equations from the $B_{(2)}$ field equation. In terms of new variables
\begin{equation}
\rho=r^2\,,\quad \widetilde{\varpi}=r^2 \varpi\,,
\end{equation}
one of them can be written as
\begin{equation}
\left(\frac{(\widetilde{\varpi}-\lambda_{\rm GB} \widetilde{\varpi} d')'}{\rho+P}\right)'=0\,,
\end{equation}
where primes denote derivatives with respect to $\rho$.  The boundary condition of \eqref{bc} leads to
\begin{equation}
\widetilde{\varpi}=\frac{J}{2(1-\lambda_{\rm GB} d')}\,.
\end{equation}
We have chosen the integration constant to agree with \eqref{CLs} in the $\lambda_{\rm GB}\to 0$ limit. Using conservation of electric charge, the equation for $d$ can also be easily derived. We find it can be integrated once more and leads to
\begin{equation}
(Q+\rho)d-\rho+\frac{\lambda_{\rm GB}}2 \left[\frac{2P\rho d'}{P+\rho}-\frac{P^2d}{(P+\rho)^2}\right]=0\, .
\label{deqn}
\end{equation}
We see that the system has been reduced to a single ordinary differential equation for $d(\rho)$.  Note that, up to a trivial overall factor, there is a scaling symmetry under
\begin{equation}
(\lambda_{\rm GB} , Q, P, \rho, d) \rightarrow (t \lambda_{\rm GB} , t Q, t P, t \rho, d) ,
\end{equation}
for constant $t$.  In the purely electric case $P=0$ the contribution from the Gauss--Bonnet invariant vanishes. However, in this case the solution is singular at $\rho=0$, so we assume that $P > 0$ in the discussion below.  To explicitly solve \eqref{deqn}, we can rewrite it as
\begin{equation}
\lambda_{\rm GB} P (\rho^{Q/\lambda_{\rm GB} - 1/2} \sqrt{\rho + P} \expe{(\rho + Q + P)^2/2 P \lambda_{\rm GB}} d(\rho))' = \rho^{Q/\lambda_{\rm GB} - 1/2} (\rho + P)^{3/2} \expe{(\rho + Q + P)^2/2 P \lambda_{\rm GB}} ,
\end{equation}
and so the general solution for $d(\rho)$ can be expressed as a integral. If there is a horizon at $\rho = \rho_0>0$, then $d(\rho_0) = 0$ and the solution exhibits a curvature singularity at $\rho=\rho_0$. At the same location, the dilaton field $L$ also diverges. Therefore, for regular solutions, the lower end of $\rho$ can always reach 0. We will not consider negative $\rho$ for the positivity of the dilaton field (string coupling constant). As \eqref{deqn} is a linear ODE with a source, its solution can be expressed a linear combination of the solution to the homogeneous equation and the special solution dictated by the source. Near $\rho=0$, the solution is approximated by
\begin{equation}
d(\rho)\sim \rho^{\frac{1}{2}-\frac{Q}{\lambda_{\rm GB} }}\left( c+\frac{2\rho^{\frac{1}{2}+\frac{Q}{\lambda_{\rm GB} }}}{2Q+\lambda_{\rm GB}} \right)\,,
\label{appsol}
\end{equation}
from which we can see when $Q/\lambda_{\rm GB} > -1/2$, the first term in \eqref{appsol} dominates and signals a curvature singularity at $\rho=0$, unless we set the integration constant $c$ to 0. On the other hand, when $Q/\lambda_{\rm GB} < -1/2$, the second term in \eqref{appsol} dominates and the solution approaches an AdS$_3$ throat. In summary, imposing regularity of the solution, we have
\begin{equation}
d(\rho) \sim \frac{\rho}{Q + \lambda_{\rm GB}/2}\,.
\end{equation}
This leads to the horizon value of the dilaton field given by
\begin{equation}
L\vert_H=\frac{Q + \lambda_{\rm GB}/2}{P}\,,
\end{equation}
whose positivity constrains
\begin{equation}
Q + \lambda_{\rm GB}/2>0\,.
\label{c1}
\end{equation}
The overlap between \eqref{c1} and $Q/\lambda_{\rm GB} > -1/2$ implies $\lambda_{\rm GB}\ge0$. In this case, the exact solution can be expressed as
\begin{equation}
d(\rho) = \frac{\rho ^{1/2 - Q/\lambda_{\rm GB}} \expe{- (\rho + Q + P)^2/2 \lambda_{\rm GB}  P}}{\lambda_{\rm GB} P \sqrt{P+\rho }}\int_0^\rho \! d y \, y^{Q/\lambda_{\rm GB} - 1/2} (y + P)^{3/2} \expe{(y + Q + P)^2 /2 \lambda_{\rm GB} P} .
\label{sol}
\end{equation}
In the other case, \eqref{c1} and $Q/\lambda_{\rm GB} < -1/2$ can be simultaneously satisfied for negative $\lambda_{\rm GB}$ whose magnitude is bounded above by $2Q$. In this case, the exact solution can be expressed as
\begin{equation}
d(\rho) =-\frac{\rho ^{1/2 - Q/\lambda_{\rm GB}} \expe{- (\rho + Q + P)^2/2 \lambda_{\rm GB}  P}}{\lambda_{\rm GB} P \sqrt{P+\rho }}\int_\rho^{\infty} \! d y \, y^{Q/\lambda_{\rm GB} - 1/2} (y + P)^{3/2} \expe{(y + Q + P)^2 /2 \lambda_{\rm GB} P} .
\label{sol}
\end{equation}
In both cases, $d(\rho) \rightarrow 1$ as $\rho \rightarrow \infty$, and in particular
\begin{equation}
d(\rho)=1-\frac{Q}{\rho}+\frac{Q^2}{\rho^2}+\cdots\,,
\end{equation}
which implies that the conserved charges measured at infinity are not modified by the inclusion of the Gauss--Bonnet combination.

\section{AdS$_3$/CFT$_2$}

Upon taking the $r\to 0$ near-horizon limit, the rotating dyonic string solution becomes a locally AdS$_3\times$S$^3$ background supported by an anti-self-dual three-form flux and a constant dilaton \cite{CL}. Local coordinate transformation brings the AdS$_3$ to the standard Ba\~{n}ados--Teitelboim--Zanelli (BTZ) black hole metric. We thus have BTZ$\times$S$^3$ as an exact solution to the $D=6$ supergravity extended by the Gauss--Bonnet combination,
\begin{align}
\label{NHS}
ds^2_6&=-\frac{(r^2-r^2_+)(r^2-r_-^2)}{\ell^2r^2}d\tau^2+r^2 \bigg( dy-\frac{r_-r_+}{\ell r^2}d\tau \bigg) ^2+\frac{\ell^2 r^2}{(r^2-r^2_+)(r^2-r_-^2)}dr^2+\ell^2ds_{{\rm S}^3}^2\,,\nonumber \\
H_{(3)}&=2\ell^2\left(\Omega_{{\rm AdS}_3}+\Omega_{{\rm S}^3}\right)\,,\qquad L=L_0\,,\qquad \ell^2=P\,,
\end{align}
where the constant $L_0$ is the horizon value of the dilaton field determined from the full asymptotically flat string solution. $r_\pm$ are the outer and inner horizon radii and $\Omega_{{\rm AdS}_3}$ and $\Omega_{{\rm S}^3}$ are the volume forms of the unit-radius AdS$_3$ and S$^3$ respectively.
It has been checked \cite{BNOPT} that this form of the horizon geometry \eqref{NHS} is preserved under the inclusion of any curvature-squared super-invariant. The off-shell relation \eqref{sol1} also guarantees that the size of the AdS radius is set by the magnetic charge $P$. Thus, for the near-horizon geometry \eqref{NHS}, only $L_0$ is model-dependent. Below, we shall compute the BTZ black hole entropy encoding the central charges of the  asymptotic Virasoro symmetry algebra, assuming the Brown--Henneaux boundary condition, via
\begin{equation}
S_{\rm BTZ}=\frac{\pi^2\ell}{3}\left(c_LT_L+c_RT_R\right)\,,\quad T_L=\frac{r_+-r_-}{2\pi\ell^2}\,,\quad T_R=\frac{r_++r_-}{2\pi\ell^2}\,.
\label{s2}
\end{equation}
On the other hand, if the model enjoys a string theory origin, the central charges can also be computed microscopically using the $D=2$ CFT description of string theory in AdS$_3$. Comparison of the macroscopic and microscopic results then furnishes a precision test of the AdS$_3$/CFT$_2$ correspondence.

We begin with the most general $R+R^2$ action preserving ${\cal N}=(1,0)$ supersymmetry in $D=6$ \cite{BNOPT}
\begin{equation}
S_{R+R^2}=\frac1{16\pi G_6}\int d^6x \left({\cal L}_{\rm EH}+\frac{1}{16}\lambda_{\rm GB}\,{\cal L}_{\rm GB}+\frac{1}{16}\lambda_{{\rm Riem}^2}\,{\cal L}_{{\rm Riem}^2}+\lambda_{R^2}\,{\cal L}_{R^2}\right)\,,
\label{IIAK3}
\end{equation}
where the supersymmetric Riemann-squared action ${\cal L}_{{\rm Riem}^2}$ takes the form \cite{BSS86,BR87}
\begin{equation}
{\cal L}_{{\rm Riem}^2}= \sqrt{-g} [ R_{\mu\nu\alpha\beta}(\omega_-) R^{\mu\nu\alpha\beta}(\omega_-)- \ft14 \epsilon^{\mu\nu\rho\sigma\lambda\tau} B_{\mu\nu} R_{\rho\sigma}{}^{\alpha}{}_{\beta} (\omega_-) R_{\lambda\tau}{}^{\beta}{}_{\alpha}(\omega_-)+\ldots ] \,,
\end{equation}
in which $R_{\mu\nu}{}^{\alpha}{}_{\beta} (\omega_-)$ is the curvature associated with the torsionful spin connection
\begin{equation}
\omega_{-\mu}^{\alpha}{}_{\beta}:=\omega_{\mu}^\alpha{}_\beta-\ft12H_{\mu}{}^\alpha{}_\beta\,.
\end{equation}
The last term in \eqref{IIAK3} denotes the supersymmetric Ricci scalar squared action whose explicit form can be found in \cite{BNOPT,O}. When auxiliary fields are switched off, which is the case considered here, ${\cal L}_{R^2}$ becomes the square of the dilaton field equation and thus does not contribute to on-shell quantities. We notice that the dilaton field only appears in ${\cal L}_{\rm EH}$, dropping out completely from the curvature-squared actions. This structure resembles the string theory low energy effective action with one-loop corrections. Indeed, if choosing
\begin{equation}
\lambda_{\rm GB}=g_s^2\ell_s^2\,,\quad \lambda_{{\rm Riem}^2}=g_s^2\ell_s^2\,,
\label{coef}
\end{equation}
the action \eqref{IIAK3} matches with the low energy effective action of type IIA string theory compactified on a K3 manifold \eqref{IIAK3} up to Ricci scalar squared terms that cannot be fixed by using string scattering amplitudes. K3 compactification of the type IIA string preserves sixteen supercharges, meaning that the particular combination with \eqref{coef} enhances the supersymmetry from ${\cal N}=(1,0)$ to ${\cal N}=(1,1)$. In our parametrization, the coefficients in front of the one-loop terms contain the string coupling $g_s$ because there is also a factor of $g_s^2$ hidden in the definition of $G_6$. The $D=6$ string coupling is determined by the asymptotic value of the dilaton field $L$.

BTZ black hole entropy in higher-derivative extended gravity models has been widely studied using the Iyer--Ward \cite{IW} formula and its generalizations concerning Chern--Simons type terms without manifest gauge invariance \cite{Tachikawa:2006sz,ALNR}.  In contrast to the non-supersymmetric models, supersymmetric completion of the Riemann tensor-squared necessary requires a $B\wedge R_\pm\wedge R_\pm$ term, which can also be recast as $H\wedge CS(\omega_\pm)$. The former is manifestly invariant under coordinate transformations and local frame rotation, but transforms non-trivially under the one-form gauge symmetry of $B_{(2)}$.  The latter is exactly the opposite. These two different choices differing in a non-gauge invariant total derivative term yields different contributions to the black hole entropy. A na\"{\i}ve application of the Iyer--Ward \cite{IW} formula to the $B\wedge R_\pm\wedge R_\pm$ term produces a vanishing result as the resulting entropy formula is proportional to $R_{\mu\nu}{}^{\alpha}{}_{\beta} (\omega_\pm)$ vanishing on the solution \eqref{NHS}. However, using the Tachikawa formula \cite{Tachikawa:2006sz}, we do get a contribution proportional to $r_-$. The apparent ambiguity can be avoided by using an approach based on dimensional reduction. As the geometry is a product space of AdS$_3$ and S$^3$, it is more natural to use the three-dimensional effective action describing the dynamics in the non-compact AdS direction. Such an action should come from reducing the six-dimensional action on S$^3$. The validity of applying this approach is supported by computing the on-shell action of the AdS$_3\times$S$^3$ solution. One obtains the correct leading contributing from the $D=3$ Einstein--Hilbert action reduced from $D=6$, in contrast to the vanishing result obtained from the $D=6$ action. As for the contributions to black hole entropy from the parity-even part of the action \eqref{IIAK3}, the computation can still be done in $D=6$ or $D=3$ using the Iyer--Wald formula. The results are identical as the near-horizon geometry \eqref{NHS} solves the field equations derived from only the parity-even part of the action \eqref{IIAK3} and conserved charges are preserved by consistent dimensional reduction. Analogous to \cite{LPS}, in the reduction we retain the metric components in the three non-compact directions, the dilaton and the scalar field parametrizing the fluctuation of $H_{(3)}$ in the non-compact directions, which are sufficient to capture the BTZ$\times$S$^3$ solution \eqref{NHS}. The reduction of $B\wedge R\wedge R$ terms in \eqref{IIAK3} then give rise to
the Lorentz Chern--Simons action. Explicitly,
\begin{equation}
-\frac{g_s^2\ell^2_s}{16\pi G_6}\int d^6x \sqrt{-g}\ft1{64}\left(\epsilon^{\mu\nu\rho\sigma\lambda\tau} B_{\mu\nu} R_{\rho\sigma}{}^{\alpha}{}_{\beta} (\omega_-) R_{\lambda\tau}{}^{\beta}{}_{\alpha}(\omega_-)+\epsilon^{\mu\nu\rho\sigma\lambda\tau} B_{\mu\nu} R_{\rho\sigma}{}^{\alpha}{}_{\beta} (\omega_+) R_{\lambda\tau}{}^{\beta}{}_{\alpha}(\omega_+)\right)
\end{equation}
reduces to
\begin{equation}
\frac{g_s^2\ell^2_s}{16\pi G_3\ell}I_{\rm CS}\,,\quad I_{\rm CS}=\frac{1}{2} \int d^3x \sqrt{-g} \epsilon^{\lambda\mu\nu}\Gamma^{\rho}_{\lambda\sigma}( \partial_{\mu}\Gamma^{\sigma}_{\rho\nu}
+\ft23\Gamma^{\sigma}_{\mu\tau}\Gamma^{\tau}_{\nu\rho} ) \,,\quad \frac{1}{G_3}=\frac{2\pi^2\ell^3}{G_6}\,,
\label{podd}
\end{equation}
to which the formula in \cite{Tachikawa:2006sz} can be applied straightforwardly.

To complete the stringy corrections to the BTZ black hole entropy, we also need the horizon value of the dilaton field in the dyonic string solution corrected by both the Gauss--Bonnet and the Riemann tensor squared term. The calculation resembles the one carried out in the previous section. We thus omit the details, but simply give the result
\begin{equation}
L\vert_{r=0}=\frac{Q}P+\frac{\lambda_{\rm GB}+\lambda_{{\rm Riem}^2}}{2P}=\frac{Q}P+\frac{g_s^2\ell_s^2}{P}\,.
\end{equation}
Summarizing contributions from various terms in the $R+R^2$ action \eqref{IIAK3}, we obtain the entropy of BTZ black boles embedded in the K3 compactification of the type IIA string,
\begin{equation}
S_{\rm BTZ}=\frac{\pi^3\ell^3}{G_6}\left[ \bigg( \frac{Q}P+2\frac{g_s^2\ell_s^2}{\ell^2}\bigg) r_+ +\frac{g_s^2\ell_s^2}{\ell^2}r_-\right]\,.
\label{s1}
\end{equation}
The Iyer--Wald formula derived from the 6D pure gravitational Gauss--Bonnet term vanishes when evaluated on the BTZ$\times$S$^3$ solution \eqref{NHS}. The additional contribution proportional to $r_+$ comes from the $RH^2$ terms that appear in the supersymmetric completion of the Gauss-Bonnet term. Comparing \eqref{s1} to \eqref{s2}, we read off the two central charges
\begin{equation}
c_L=\frac{3\pi^2\ell^4}{G_6}\left(\frac{Q}{P}+\frac{g_s^2\ell_s^2}{\ell^2}\right)\,,\quad c_R=\frac{3\pi^2\ell^4}{G_6}\left(\frac{Q}{P}+3\frac{g_s^2\ell_s^2}{\ell^2}\right)\,.
\label{cc}
\end{equation}

Upon lifting to type IIA string theory, the rotating string solution is composed of a bound state of $N_1$ fundamental strings and $N_5$ NS5-branes wrapped on K3. Therefore, the electric and magnetic energies carried by the asymptotically flat rotating string solution \eqref{genstr} should match with those of fundamental strings and NS5-branes. Using the fact that a NS5-brane wrapped on K3 becomes
a solitonic string in $D=6$ with effective tension
\begin{equation}
T_{\rm NS5}{\rm Vol}(K3)\,,\quad T_{\rm NS5}=\frac{1}{(2\pi)^5g_s^2\ell_s^6}\,,\quad {\rm Vol}( K3)=(2\pi\ell_s)^4\,,
\end{equation}
we obtain
\begin{equation}
Q=\frac{2N_1G_6}{\pi^2\ell^2_s}\,,\qquad P=\frac{2N_5G_6}{\pi^2g_s^2\ell^2_s}\,.
\label{relation1}
\end{equation}
On the other hand, the $D=6$ Newton's constant is related to the $D=10$ Newton constant $G_{10}$ via
\begin{equation}
G_6{\rm Vol (K3)} =G_{10}\,,\qquad 16\pi G_{10}=(2\pi)^7g_s^2\ell_s^8\,.
\label{relation2}
\end{equation}
Substituting \eqref{relation1}, \eqref{relation2} and $\ell^2=P$ into \eqref{cc}, we can express the central charges in terms of the quantized parameters
\begin{equation}
c_L=6N_5(N_1+1)\,,\qquad c_R=6N_5(N_1+3)\,.
\label{cc2}
\end{equation}
The geometric background is valid when the string is weakly coupled and the AdS radius is much larger than the string length, in other words, $g_s\ll1$ and $N_5\gg1$, under which the AdS radius is also much larger than the Planck length. The AdS$_3\times$S$^3\times$K3 vacuum in type IIA preserves eight chiral supercharges, which amounts into $(4,0)$ supersymmetry in $D=2$.  This means that the CFT$_2$ dual should be a $(4,0)$ SCFT with left and right $\widehat{SL(2)}\times\widehat{SU(2)}$ affine symmetry. The central charges of the dual CFT ought to match with those in the gravity side \eqref{cc2}, but we omit here an independent calculation of the central charges on the CFT side. Using the duality between the type IIA string on K3 and the heterotic string on $T^4$, we can map the solution obtained here to a solution in heterotic string theory with leading order stringy corrections. Denoting the fields in the heterotic string by $\{\widetilde{g}_{\mu\nu}\,,\widetilde{B}_{\mu\nu}\,,\widetilde{L} \}$, the $D=6$ type IIA/heterotic string duality at ${\cal O}(\ell_s^2)$ is given by \cite{LPS, LM}
\begin{equation}
\widetilde{H}_{(3)}=L*H_{(3)} \,,\qquad \widetilde{g}_{\mu\nu}=L g_{\mu\nu}\,,\qquad \widetilde{L}=L^{-1}\,,
\end{equation}
under which the low energy effective action of the type IIA string with leading one-loop corrections \eqref{IIAK3} is mapped to the effective action of the heterotic string with leading tree-level stringy corrections
\begin{equation}
\widetilde{S}=\frac1{16\pi G_6}\int d^6x\sqrt{-\widetilde{g}}\widetilde{L}[\widetilde{R}+\widetilde{L}^{-1}\nabla^\mu \widetilde{L} \, \nabla_\mu \widetilde{L} - \ft{1}{12}\widetilde{H}^{\mu \nu \rho} \widetilde{H}_{\mu\nu\rho}+\ft18\ell_s^2\widetilde{R}_{\mu\nu\alpha\beta}(\omega_+) \widetilde{R}^{\mu\nu\alpha\beta}(\omega_+)+\ldots]
\end{equation}
in which $\widetilde{H}_{(3)}$ obeys the non-trivial Bianchi identity
\begin{equation}
d\widetilde{H}=\ft14\ell_s^2{\rm tr}(\widetilde{R}_+\wedge \widetilde{R}_+)+\ldots\,.
\end{equation}
In the formulae above, we have omitted the spin-1 gauge fields, which are not relevant here. Holographic central charges for the dualized AdS$_3\times$S$^3$ solution can be readily computed by noticing a few shortcuts. Firstly, the contribution from the
Einstein--Hilbert action is unchanged because the Einstein-frame metric remains the same under the duality transformation. Secondly, the parity-odd contribution is opposite to that of \eqref{IIAK3}, since the on-shell relation $\widetilde{L}*\widetilde{H}=H$ means that there is effectively an $H\wedge {\rm CS}(\omega_+)$ term with coefficient $-\ft14\ell_s^2$. Finally,
the parity-even $\widetilde{R}_+^2$ term does not contribute, since $\widetilde{R}_+$ vanishes for the solution. We thus obtain the entropy of BTZ black boles embedded in the $T^4$ compactification of the heterotic string
\begin{equation}
\widetilde{S}_{\rm BTZ}=\frac{\pi^3\ell^3}{G_6}\left[ \bigg( \frac{Q}P+\frac{g_s^2\ell_s^2}{\ell^2} \bigg) r_+-\frac{g_s^2\ell_s^2}{\ell^2}r_-\right]\,.
\end{equation}
It is evident that the duality transformation interchanges the role of the fundamental and solitonic strings. Thus in the dualized solution, $Q$ is related to $\widetilde{N}_5$, the number of heterotic NS5-branes, while $P$ is related to $\widetilde{N}_1$, the number of heterotic fundamental strings. In terms of the quantized parameters, the central charges for the
AdS$_3\times$S$^3\times T^4$ solution in the heterotic string are expressed as
\begin{equation}
\widetilde{c}_L=6\widetilde{N}_1(\widetilde{N}_5+2)\,,\qquad \widetilde{c}_R=6\widetilde{N}_1\widetilde{N}_5\,.
\label{cc2b}
\end{equation}
The CFT dual to the heterotic string in the AdS$_3\times$S$^3\times T^4$ background was studied in \cite{KLL}. It is a $(4,0)$ SCFT with left and right $\widehat{SL(2)}\times\widehat{SU(2)}\times\widehat{U(1)}^4$ affine symmetry.
The central charges in the left and right movers are
\begin{equation}
c_L=6p(k+2)\,,\qquad c_R=6pk\,,
\label{cc3}
\end{equation}
where $p$ is the number of fundamental strings and $k$ is the level of the $\widehat{SL(2)}$ algebra in the supersymmetric right mover. The matching between \eqref{cc2b} and \eqref{cc3} leads to the identification
\begin{equation}
k=\widetilde{N}_5\,.
\label{id}
\end{equation}

\section{Conclusion and discussion}

In this paper, we proposed a method for constructing BPS
solutions in higher-derivative extended supergravity models from known solutions in two-derivative theories. Application of our method requires an off-shell formulation underlying the supergravity theory. For simplicity, we focused on 6D ungauged supergravity models involving only the dilaton--Weyl multiplet. Adding off-shell vector multiplets to the model is straightforward.  A concrete example was given by obtaining the first rotating dyonic string solution in 6D Einstein-Gauss-Bonnet supergravity, exhibiting the advantage of our method when applied to non-static solutions. An obvious generalization of our solution
is to turn on monopole charge $M$ on $S^3$. In this case, the solution respects the same U(2)$\times\mathbb{R}^2$ symmetry and remains cohomogeneity-1. The entropy of the BTZ black hole arising from the near-horizon limit of the dyonic string in monopole background will be labeled by three integers \cite{KLL}. Upon dualizing the solution from type IIA string theory to the heterotic string, we will be able to compare the gravity and dual CFT results \cite{KLL}. We would also like to apply our construction to the more intricate cohomogeneity-2 case, in particular to the smooth horizonless microstate geometries \cite{Bena:2016ypk, Bena:2017geu} that have the same asymptotic structure at infinity as a given supersymmetric black hole of the same mass, charges and angular momenta. The microstate geometries also admit an AdS$_3\times$S$^3$ throat. It would be interesting to investigate if the throat region of the microstate geometry receives the same stringy corrections as the near-horizon limit of the dyonic strings. Finally, the off-shell supersymmetric curvature-squared terms are also known in $D=4$ and $D=5$. Their component forms are explicitly given in \cite{Cecotti:1986jy}-\cite{OP2}. Some of them do not come from dimensional reduction of the 6D theories and require separate consideration. Although many stationary BPS solutions have already been discovered in the corresponding two-derivative theories, the known supersymmetric black holes in $D=4$ and $D=5$ higher-derivative extended supergravities are restricted to the static case (see e.g.\ \cite{Behrndt:1998eq,Castro:2008ne}), so there remains much to be done.

\section*{Acknowledgements}
	We are grateful to T.\ Azeyanagi, G.\ Comp\`{e}re, M.\ Duff, H.\ L\"{u}, S.\ Schafer-Nameki and J.\ Sparks for useful discussions. We also thank D.\ Kutasov and F.\ Larsen for useful correspondence. It is also a pleasure to thank D.\ Butter, J.\ Novak, M.\ Ozkan and G.\ Tartaglino-Mazzucchelli for collaborations on related projects. The work of Y.P.\ is supported by the Newton International Fellowship NF170385 of the Royal Society.

redpajama_set_name: RedPajamaArXiv


The Tokyo Rainbow Pride 2018 Festival began on April 28 and came to a close on May 6 with the much-anticipated parade after 9 whole days of consecutive events around Tokyo and its neighboring wards. Members of the LGBTQ+ community and allies alike took to the streets of Shinjuku donning every color of the rainbow to show pride and unity.
On May 5 and 6, Harajuku Station drummed with footsteps from the heavy foot traffic stepping off of the Yamanote Line train. One could argue that it was just your usual Sunday considering the dense waves of passengers the station welcomes daily; there are people on their way to work, people on a shopping excursion, and tourists sampling what Harajuku has to offer. But, this particular Sunday has set itself apart from all the other ones. The air was electric with lively conversations, and the sun was as warm as the people under it. By their clothes, these people formed a path that would've twined The Wizard of Oz's yellow brick road if only it were rainbow-colored, and the end of it was the source of the merry din: The Pride Festival.
The festivities were already in full swing at Yoyogi Park even hours before the parade. Rows and rows of tented booths occupied the venue. From foods to goodies, social media to tech, and even different organizations and businesses, attendees stopped by their set-ups to try out the services offered or deck themselves out in Pride merchandise. People were coming in and out of Shiseido's booth for a skin consultation. At Panasonic's, whose booth matched their corporate colors of black and blue, people lined up for facial hair grooming. Social media titans such as Google, Facebook, Instagram, and Buzzfeed were also present at the event and had photo booths at their tents. Food trucks and food tents offering selections of desserts and meals—such as ice cream and yakisoba to name a few—enclosed the entire venue. Nearby were eating areas where some people, with their food in hand, rested.
The clock struck 12 and, true to Japanese fashion, the Pride Parade started. Group after group, participants went out to the streets from the Shibuya Exit of Yoyogi Park to share the merrymaking to passersby. With interests piqued, onlookers gathered along sidewalks to take photos and join in on the fun by waving and giving off high-fives. As the parade made its way along Omotesando, Lush employees of the Omotesando branch cheered on from their second-story window. From there, the parade circled back to the venue.
It was almost 3 o'clock in the afternoon when the parade made its way back to Yoyogi Park, and the crowd seemed to have doubled in size. As the temperature rose over time, so did the excitement of the attendees. People still went from booth to booth, stopping only once in a while to take photos; some went for food to recharge. By the time the sun had made its way halfway west, people were positioning themselves around the stage to wait for the headliner. Famous Japanese pop idol, Ayumi Hamasaki went on, much to the crowd's cheering, and performed fan-favorites.
At around 6 pm, the performance ended; organizations who occupied the booths started to pack up, and the crowd began to disperse. Although the festivities at Yoyogi Park has finished, the night had just begun. The official closing party was held down at Shinjuku Ni-Chome's AiSOTOPE LOUNGE, and the celebration went on until midnight.


Front caster arms, factory with offset bushes inserted giving around 8 - 9 degrees castor.
Rear camber arms, ball jointed with no slop or clunks. These were only replaced because I got some Hardrace rubber bushed adjustables instead.


I have a virtual server that I'm running UNMS on. It looks good so far, but now i want to run another service on this host that also needs Port 80 and Port 443.
I can assign another IP address to the host without any problems.
How can I bind the UNMS docker instance to just one of the IP addresses on this host?
e.g. the Host has the IP address 10.0.0.10 and UNMS is happily listening on this address.
I add a second IP address, 10.0.0.20 to the same interface, and now I want UNMS to just repsond to queries on 10.0.0.10 so my other app can respond to queries on 10.0.0.20.
@kai_h Hello Kai. In order to achieve this, you would need to configure and run a Proxy server and start UNMS on a nonstandard port. It is tricky to configure the proxy properly though. If you search the community forum there may be a thread dealing with this already. Also, we have a guide for proxy servers right here.
Thank you for the reply. It seems a bit long-winded to have to configure a reverse proxy just to bind to a specific IP - is there no way to do this in the Docker configuration instead?
@kai_h Hello Kai. Right now we do not know how to accomplish this through Docker while making the solution stable in the long run. The developers came up with an idea of solving this situation with the installation script option though. We will add this in some later release.


Emma may not post as often as Ruby, but from time to time she will contribute a post about finicky felines or something for Things Worth Sharing. Mostly she likes to help behind the scenes at Kat Treats Headquarters.
She might direct the photo shoot of the finished product.
She might decide that she should review Halloween candy rather than Emma-safe treats.
Sometimes Emma might even pretend to be one of her favorite internet cats.
Mostly Emma just sits around being a pretty girl.
For all the these things and more, we wish Emma and all the other fabulous felines out there a Happy National Cat Day on October 29th.
My Ultimate Pet's Rejeneril Review and Giveaway!


text:
Czech and Austrian opponents for our Europa League teams
The draw has been made for the knock-out stage of this season's UEFA Europa League. Two Belgian clubs were among the 32 that went into the draw.
Mon 17 Dec 2018 16:07
Last season's Belgian League Champions Club Brugge qualified thanks to finishing third in their Champions' League group. Ivan Leko's men will take on the Austrian side Red Bull Salzburg. Although not one of Europe's top teams Red Bull Salzburg have dominated Austrian football in recent years, winning 5 consecutive league titles.
It will be the first ever meeting between the two clubs. However, Red Bull Salzburg have played other Belgian opponents in European competition in recent years. In 2013 the Austrians were beaten twice by Standard de Liège in the group stage of the Europa League. Standard also knocked them out of the Europa League in 2009.
Salzburg qualified from their group together with the Scottish champions Celtic. The Austrians' strikers Dabour and Gulbrandsen scored no fewer than 7 goals in the group stage.
KRC Genk to take on Slavia Prague
The league-leaders KRC Genk will take on Slavia Prague. This too will be the first time that the two clubs have met.
The Czechs qualified from a tough group consisting of Zenit Saint Petersburg (the group winners), Bordeaux and Copenhagen.
Slavia have displayed strength in defence, keeping clean sheets in 3 of their 6 group stage games.
KRC Genk will play the first leg of their tie away, while Club Brugge will play the first leg at home. The first leg games will be played on Thursday 14 February, while the return leg will be played a week later on 21 February 2019.
Golden Boot Vanaken steers Club Brugge to victory against Anderlecht
Peter De Voecht / Photo News
Antwerp come back from behind to beat Cercle
Bolcina/Photo News
AA Gent second after home win against Excel Mouscron
Standard start the year with a win


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text:
Age estimation using 2 nd molar development: An efficient indicator of adolescent age
Shweta Yellapurkar, N. Srikant, Dilip Naik, Nandita Shenoy, Vaishnavi Gundeti
Department of Oral Pathology and Microbiology, Manipal College of Dental Sciences, Mangalore
Department of Oral Medicine and Radiology, Manipal College of Dental Sciences, Mangalore
Background and objectives. Assessment of stage of Tooth development is a reliable method for age estimation. Most of the studies emphasize the use of stages of eruption of third molar in forensics and very little is known about the efficacy of the second molar. Thus, our present study we evaluated the efficacy of developmental staging of second and third molars to predict the age of ≤ 14 year old individual. Material and Methods. Digital radiographs of 404 individuals aged between 7-20 years were retrieved. 10 stages of tooth development advocated by Köhler et al. was used to assess the developmental stages of second and third molars. Regression equations were derived to estimate age using second and third molar development stages. Results. When compared to third molars, the formula derived using second molars, was seen to provide better results in identifying the adolescence status (98.4 %) when compared to childhood (63.01%). Also the estimation was better seen females than in males in distinguishing the age of >14 years. Conclusion. Thus, dental age estimation by using second molar could be a valuable indicator of age in young adults. Also, in medicolegal cases, second molars could be useful to identify children ≤14 years, could be used with other adjuvant measures.
Romanian Journal of Legal Medicine
https://doi.org/10.4323/rjlm.2018.274
Third Molar
Yellapurkar, S., Srikant, N., Naik, D., Shenoy, N., & Gundeti, V. (2018). Age estimation using 2 nd molar development: An efficient indicator of adolescent age. Romanian Journal of Legal Medicine, 26(3), 274-278. https://doi.org/10.4323/rjlm.2018.274
Yellapurkar, Shweta ; Srikant, N. ; Naik, Dilip ; Shenoy, Nandita ; Gundeti, Vaishnavi. / Age estimation using 2 nd molar development : An efficient indicator of adolescent age. In: Romanian Journal of Legal Medicine. 2018 ; Vol. 26, No. 3. pp. 274-278.
@article{835e225827934d1c8388c5537bc519a0,
title = "Age estimation using 2 nd molar development: An efficient indicator of adolescent age",
abstract = "Background and objectives. Assessment of stage of Tooth development is a reliable method for age estimation. Most of the studies emphasize the use of stages of eruption of third molar in forensics and very little is known about the efficacy of the second molar. Thus, our present study we evaluated the efficacy of developmental staging of second and third molars to predict the age of ≤ 14 year old individual. Material and Methods. Digital radiographs of 404 individuals aged between 7-20 years were retrieved. 10 stages of tooth development advocated by K{\"o}hler et al. was used to assess the developmental stages of second and third molars. Regression equations were derived to estimate age using second and third molar development stages. Results. When compared to third molars, the formula derived using second molars, was seen to provide better results in identifying the adolescence status (98.4 {\%}) when compared to childhood (63.01{\%}). Also the estimation was better seen females than in males in distinguishing the age of >14 years. Conclusion. Thus, dental age estimation by using second molar could be a valuable indicator of age in young adults. Also, in medicolegal cases, second molars could be useful to identify children ≤14 years, could be used with other adjuvant measures.",
author = "Shweta Yellapurkar and N. Srikant and Dilip Naik and Nandita Shenoy and Vaishnavi Gundeti",
doi = "10.4323/rjlm.2018.274",
journal = "Romanian Journal of Legal Medicine",
publisher = "Romanian Legal Medicine Society",
Yellapurkar, S, Srikant, N, Naik, D, Shenoy, N & Gundeti, V 2018, 'Age estimation using 2 nd molar development: An efficient indicator of adolescent age', Romanian Journal of Legal Medicine, vol. 26, no. 3, pp. 274-278. https://doi.org/10.4323/rjlm.2018.274
Age estimation using 2 nd molar development : An efficient indicator of adolescent age. / Yellapurkar, Shweta; Srikant, N.; Naik, Dilip; Shenoy, Nandita; Gundeti, Vaishnavi.
In: Romanian Journal of Legal Medicine, Vol. 26, No. 3, 01.09.2018, p. 274-278.
T1 - Age estimation using 2 nd molar development
T2 - An efficient indicator of adolescent age
AU - Yellapurkar, Shweta
AU - Srikant, N.
AU - Naik, Dilip
AU - Shenoy, Nandita
AU - Gundeti, Vaishnavi
N2 - Background and objectives. Assessment of stage of Tooth development is a reliable method for age estimation. Most of the studies emphasize the use of stages of eruption of third molar in forensics and very little is known about the efficacy of the second molar. Thus, our present study we evaluated the efficacy of developmental staging of second and third molars to predict the age of ≤ 14 year old individual. Material and Methods. Digital radiographs of 404 individuals aged between 7-20 years were retrieved. 10 stages of tooth development advocated by Köhler et al. was used to assess the developmental stages of second and third molars. Regression equations were derived to estimate age using second and third molar development stages. Results. When compared to third molars, the formula derived using second molars, was seen to provide better results in identifying the adolescence status (98.4 %) when compared to childhood (63.01%). Also the estimation was better seen females than in males in distinguishing the age of >14 years. Conclusion. Thus, dental age estimation by using second molar could be a valuable indicator of age in young adults. Also, in medicolegal cases, second molars could be useful to identify children ≤14 years, could be used with other adjuvant measures.
AB - Background and objectives. Assessment of stage of Tooth development is a reliable method for age estimation. Most of the studies emphasize the use of stages of eruption of third molar in forensics and very little is known about the efficacy of the second molar. Thus, our present study we evaluated the efficacy of developmental staging of second and third molars to predict the age of ≤ 14 year old individual. Material and Methods. Digital radiographs of 404 individuals aged between 7-20 years were retrieved. 10 stages of tooth development advocated by Köhler et al. was used to assess the developmental stages of second and third molars. Regression equations were derived to estimate age using second and third molar development stages. Results. When compared to third molars, the formula derived using second molars, was seen to provide better results in identifying the adolescence status (98.4 %) when compared to childhood (63.01%). Also the estimation was better seen females than in males in distinguishing the age of >14 years. Conclusion. Thus, dental age estimation by using second molar could be a valuable indicator of age in young adults. Also, in medicolegal cases, second molars could be useful to identify children ≤14 years, could be used with other adjuvant measures.
U2 - 10.4323/rjlm.2018.274
DO - 10.4323/rjlm.2018.274
JO - Romanian Journal of Legal Medicine
JF - Romanian Journal of Legal Medicine
Yellapurkar S, Srikant N, Naik D, Shenoy N, Gundeti V. Age estimation using 2 nd molar development: An efficient indicator of adolescent age. Romanian Journal of Legal Medicine. 2018 Sep 1;26(3):274-278. https://doi.org/10.4323/rjlm.2018.274
10.4323/rjlm.2018.274


(in. N. Transept, brass). Magistratus indicat virum. Henry Earl of Lonsdale, Lord Lieutenant and Custos Rotulorum of Westmoreland & Cumberland, Colonel of the Westmorland and Cumberland Yeomanry Cavalry, Hon: Colonel of the Royal Cumberland Militia, Hon: Colonel of the Cumberland Volunteers, late Captain in the 1st Life Guards. Rep. Westmoreland in Parliament 25 years. B. Mar: xxvii A.D. mdcccxviiiD. Aug: xv A.D. mdccclxxvi. To whose beloved memory, the best of husbands and fathers and the most upright of gentlemen, this monument is erected by his wife. The memory of the just is blessed. (This is on either side of a full length figure, full face, in uniform of the 1st Life Guards, holding the helmet in the right hand; being a portrait of Henry Lord Lonsdale. Mr. Grump). Two shields of Arms (above), 1. or. 6 annulets 3, 2, I, sa. (Lowther) (with ulster badge). 2. Lowther impaling barry of 10 ar. & gu. on canton of 2nd lion passant guardant or (Caulfeild). Also 2 medallions each containing 5 small shields. On 1st medallion are I. Lowther (with ulster badge); II. Sa. 3 escallops within bordure engrailed ar. (Strickland); III. Gu. 3 lucies hauriant or (Lucy); IV. Ar. lion rampant sa. (Stapleton); V. Erm. on canton az. cross calvary or, (Quaile). On 2nd medallion, I. Sa.3 covered cups ar. (Warcop); II. Sa. 3 martlets volant ar. (Coll. Arms C. 39, 15 born ); III. Ar. 2 bars gu. on canton of 2nd, mullet of the field (Lancaster of Sockbridge); IV. Ar.3 bugle horns sa. (Bellingham); V. Ar. chevron gu. between 3 torteaux (Sherard).


The Marionne grandad-collar shirt in white is a contemporary take on a wardrobe classic. It's woven from a pure-cotton fabrication and cut to a regular fit. Team it with a tailored navy suit and monk strap shoes for a refined tailored look.


text:
Q: jQuery element selector after appends I selected my elements after appends. But I can't do anything inside of the click function. Here's my code:

     //content is here after appends

data (div-3 is hidden):

          Label

          Text

  ...

jQuery (I want to show div-3 on mousehover and then hide the span in div-2 and then create input or show input in div-2, after that I will update the value in that input):
$(function(){

            $('.main').on('mouseover', '.data_list li', function () {
                $(this).find('.div-3').show();

                $('.main ').on('mouseout', '.data_list li', function () {
                    $(this).find('.div-3').hide();

                });
            });
            $('.main').on('click', '.data_list .div-3 a', function () {
                // I don't know what can I do here.
               //I want to hide the span in div-2 and create a forminput instead.
              //I tried $(".div-2 span").hide(); but didn't work.
            });

        })

A: You can select the class that is assigned to that 'a' element
$('.edit').on('click', function () {
    //code to be executed
}

I would build the input into my html, set it as hidden in your css, and then show it using jquery.
HTML

    Text
    <input class="list-input">

CSS
.list-input {
   display: none;
}

JQUERY
$('.list-input').show();

redpajama_set_name: RedPajamaStackExchange


After connecting to the server via SSH I start screen (without options). Then, no matter if I close my terminal application (iTerm or Terminal, by clicking on "the x" or via CMD+W ) or detach the screen session first using CTRL+A D, in any case the screen process gets killed and the session is gone. For debugging, I have explicitly set autodetach to on now, but that does not help.


Katie has been clerking since 2009 and is now the Practice Manager to the Criminal Law team, with responsibility for the day to day management of the Bournemouth centre diary. She deals with all fees for both prosecution and defence work and handles any client queries. She is also the Bournemouth Centre Manager.
Prior to joining 3PB, she was a Crown Court Clerk at a firm of local solicitors that specialised in criminal defence work.


text:
Kyoung H. Park
My central question as a theater-maker is how can the performing arts help us create a culture of peace? Through playwriting, intercultural, community-based dialogues, and interdisciplinary collaborations, I challenge artists and audiences to find new ways and forms of expression, to search for answers and truths that may not exist, or that may require new language for it to be articulated. I reach towards the limits of my own understanding in order to force myself into a state of imagination, invention and creation– of world peace. I find this both optimistically naive and seriously ridiculous; tonally, my work comes across as both.
Kyoung H. Park is a North Korean playwright/director, born and raised in Santiago, Chile, currently living in unceded territory of the Lenape. As Artistic Director of Kyoung's Pacific Beat, he has devised three full-length plays — disOriented, TALA, and PILLOWTALK, created over 35 community-based, experimental projects including performances for new media, and is author of Sex and Hunger, Walkabout Yeolha, and many short plays including Mina, which is published in Seven Contemporary Plays from the Korean Diaspora in the Americas by Duke University Press. Kyoung's work centers stories of (im)migration, queerness, trauma, and the ways these intersect in communities of color; it's described as "intensely personal" by American Theater Magazine and "very much of this moment" by the New York Times.
Kyoung's Pacific Beat has been a resident company at The Tank, Bushwick Starr, Baryshnikov Arts Center, New Ohio, BRIC Arts Media, LaGuardia Performing Arts Center, Performance Project @ University Settlement and Kyoung has been International Exchange Fellow at Augusto Boal's Theatre of the Oppressed, Writer-in-Residence at Sanskriti Pratisthan (New Delhi), Vermont Studio Center, Centro Cultural Gabriela Mistral (Santiago, Chile) and he is a member of the Ma-Yi Writer's Lab, NYTW Usual Suspect, and co-founder of The Sol Project. He is currently a Steering Committee member of the Mosaic Network and Fund, Advisory Council member of HueArts NYC, and 2022 APAP Conference Committee member.
Before founding Kyoung's Pacific Beat, Kyoung co-directed workshop productions of Lee Breuer's LA DIVINA CARICATURA (PS122, Public Theater's Under the Radar Festival), MABOU MINES' GLASS GUIGNOL (Provincetown's Tennessee Williams Theater Festival, Sundance Theater Institute at Mass MoCA, Wesleyan University, St. Ann's Warehouse), interned for Young Jean Lee's Theater Company (LEAR, Soho Rep) and 13P (WE'RE GONNA DIE, Joe's Pub), and is an alum of the Royal Court Theatre's Young Writer's Programme (London), Ensemble Studio Theatre's Youngblood, and Soho Theatre's Writer's Hub (London).
Kyoung is recipient of numerous fellowships including the 2021 Jerome Hill Artist Fellowship (Recommended Alternate), 2021 New York Foundation for the Arts Incubator for Executive Leaders of Color, 2019-2020 Dramatist Guild Fellowship, 2019-2020 Target Margin Arts Management Fellowship, 2018-2020 APAP Leadership Fellowship, 2018-2019 Intercultural Leadership Institute Fellowship, 2017 Creative Mellon Fellowship, 2015-2017 Field Leadership Fund Fellowship, 2014 Target Margin Theater Inst. for Theater-Making Fellowship, and was named a 2010 UNESCO-Aschberg Laureate (Paris). He is recipient of commissions from Mixed Blood Theater Company (Minneapolis), Latinx Theater Commons/Howlround (New York) and Kyoung has received grants from the Arvon Foundation (London), GK Foundation (South Korea), MAP Fund, Venturous Theater Fund, TCG Global Connections, Brooklyn Arts Council, Howard Gilman Foundation, Foundation for Contemporary Arts Emergency Grant, and has been a grant panelist for the NEA, TCG, ART/NY and NALAC.
Kyoung lives in Brooklyn, New York with his husband, Daniel Lim, and continues his self-education in Buddhism, having made his refuge vows with His Holiness the 14th Dalai Lama in Dharamsala, India. He holds an MFA in Playwriting from Columbia University (Dean's Fellow), MA in Peace and Global Governance from Kyung Hee University's Graduate Institute of Peace Studies, and BFA in Dramatic Writing from NYU (Founder's Day Award).
"BIPOC Affinity Space," Co-Facilitator, Association of Performing Arts Professionals, New York City. Jan. 9, 2021
"Redistribution of Power: Building Radical Collective Action," Mosaic Fund and Network / Kyoung's Pacific Beat, New York City. Oct. 13, 2020
"Redistribution of Power: Imagine Forward," Mosaic Fund and Network / Kyoung's Pacific Beat, New York City. Sept. 17, 2020
"Redistribution of Power: Addressing the Urgency of Now," Mosaic Fund and Network / Kyoung's Pacific Beat, New York City. Aug. 19, 2020
"Building Community Care Platforms for the Indie Theater Community," New York, May 4, 2020
"Building Community Care Strategies for the Indie Theater Community," New York, Mar. 23, 2020
"How Artists and Presenters do Anti-Oppression Work," Association of Performing Arts Professionals (APAP) Conference, New York, Jan. 13, 2020
"Intercultural Leadership PreConference," Intercultural Leadership Institute at Americans for the Arts Annual Convention, Minneapolis, Jun. 13-14, 2019
"Asian-Americans for Equality's 8th Annual Youth Career Conference", Asian-Americans for Equality, New York, NY. Apr. 13, 2019
"Feminist Perspectives on Building Intersectional Communities", Kyoung's Pacific Beat, Chicago, IL. Aug. 17, 2018
"International Devised Theater Conference", The Dramatists Guild of America, New York, NY. Jul. 28, 2018
"Opening Night: Arts Showcase", KQTcon- A National Conference for Queer and Trans Korean Americans, New York, NY. Apr. 6, 2018
"Activate Equity", The Field, New York, NY. Mar. 17, 2018
"Marriage Equality Across the Generations", Kyoung's Pacific Beat, New York, NY. Jan. 13, 2018
"The Creative Process: Artist-Driven Transformational Research", APAP/NYC 2018, New York, NY. Jan. 13, 2018
"Meeting a Distant Star", Abrons Arts Center, New York, NY. Sept. 28th, 2017
"Literature and Social Practice", Ehwha Women's University, Seoul, South Korea. July 2017
"Colaboracion Experimental", Teatro DUOC, Santiago, Chile. June 2017
"Art for Change: A Panel Discussion", Asian-American Arts Alliance, New York, NY. Dec. 8, 2016
"Politics, Revolution, and Art: A Theatrical Symposium", Woolly Mammoth Theatre Company, The Laboratory for Global Performance and Politics, Global Theater Initiative in association with the Middle East Institute's Arts and Cultural Program, Washington, DC. Nov. 5, 2016
"Creating Peace Through Art", Korea Arts Council – Artist House, Seoul, South Korea. Oct. 21, 2016
"Devising Outside the Box", Seismic Shifts: 5th National Asian American Theater Conference & Festival at Oregon Shakespeare Festival, Ashland. Oct. 3, 2016
"Creating Peace Through Art", Hot Asian Everything: A Seismic Exhibition, Mulnomah County Library, Portland. Oct. 2, 2016
"Finding Home: Migration, Exile and Belonging," TCG Global Pre-Conference at George Washington University, Washington, DC. Jun. 22, 2016
"Morley: Circle Round Dignity, Courage & Survival," David Rubenstein Atrium at Lincoln Center. Apr. 27, 2016
"Checkpoints: Communication Consciousness." NYC Asian-American Student Conference, New York University. Mar. 14, 2016
"Dreaming the Americas—Cultural Appropriation- Who's Telling Whose Story" NoPassport Conference. New York University. Mar. 14, 2016
"LabEscenico," Festival Santiago a Mil / Theater Communications Group (TCG). Santiago, Chile. Jan. 22, 2016
"Dramaturgia Experimental," Interdram at Matucana 100. Santiago, Chile. Dec. 21-29, 2015
"Open Spectrum Critical Community Dialogues: Navigating Privilege," Culturebot / MAPP International Productions. New York Live Arts. Dec. 7, 2015
"The Conscious Language In Practice," Poetic Theater Productions. Wild Project Theater, NYC. Aug. 29, 2015
"Healing Political Trauma," Kyoung's Pacific Beat. Performance Project @ University Settlement. Jan. 15, 2015
"Latino Commons Encuentro," Martin Segal Center, CUNY. Nov. 10, 2014
"Queering Gay Marriage," Kyoung's Pacific Beat. Ma-Yi Studio. Jun. 2, 2014
"The Uncomfortable Conversation," Brooklyn Commune Global Congress. Invisible Dog Center, NYC. Nov. 22, 2013
"On the Nature of Political Revolutions," Kyoung's Pacific Beat. HERE Arts Center. Jul. 29, 2012
"North Korea: WTF?" Kyoung's Pacific Beat. Theater C @ Peter Jay Sharp Theater on 42nd Street. Feb. 26, 2011.
Asian/Pacific/American Institute at New York University, A/P/A Voices: A COVID-19 Public Memory Project. Jan. 2021 – Present
Mosaic Fund and Network, Steering Committee Member. Apr. 2020 – Present
Indie Theater Fund, Board Member. Apr. 2019 – Apr. 2020
Sol Project, Advisor, Co-Founding Member. Aug. 2014 – Present
The Dramatist Guild, Devised Theater Committee Member. Apr. 2016 – Jul. 2018
Performance Project @ University Settlement, Artistic Advisory Board. May 2016 – May 2017
Brooklyn Commune, Director of Cultural Democracy and Representation Research Team. May 2013 – Nov. 2014
Second Generations, Director of Strategic Planning, Program Director for Community Voices: Queer API. Aug. 2012 – July 2013
GAPIMNY, Fundraising Chair. Aug. 2011 – Dec. 2013


The problem with mouse click noises is that they are totally unnecessary in terms of providing feedback to the user (assuming that the user doesn't have some kind of physical/mental disability how to make jam doughnuts video Solution 1: Make sure "Integrate 7-Zip to shell context menu" option is checked Step 1: Open Windows 10 Start menu. Type 7zip in the search box, and then in the search result, right-click on the 7-Zip File Manager and select Run as administrator .
6/07/2014 · I would like to know how I can make it so that I don't hear my mouse clicking while I am recording. The clicking is pretty annoying while trying to watch the recording. how to make mickey mouse drawing They found it difficult to make a mouse that does not make a clicking-sound. However they have found some patented silent switches and integrated them into a stylish but practical wireless mouse. However they have found some patented silent switches and integrated them into a stylish but practical wireless mouse.
They found it difficult to make a mouse that does not make a clicking-sound. However they have found some patented silent switches and integrated them into a stylish but practical wireless mouse. However they have found some patented silent switches and integrated them into a stylish but practical wireless mouse.
6/07/2014 · I would like to know how I can make it so that I don't hear my mouse clicking while I am recording. The clicking is pretty annoying while trying to watch the recording.


text:
Q: TTCE-K750 Card DISPENSER WITH RECYCLABLE APPLICATION I am using the rfid card dispenser module which is connected as usb serial and certain commands are are passed to get senor status using the following serial communication data but issue is we can't able to find any status for card insertion in sensor status is there a way to find this status from the dispenser sensors as below
fun getStatus(context: Context,type: String) {
            val nRet: Int
            val StateInfo = ByteArray(4)
            val SendBuf = ByteArray(3)
            val RecordInfo = arrayOfNulls<String>(2)
            nRet = if (Connectflag) {
                k720_usb!!.K720_SensorQuery(MacAddr, StateInfo)
            } else {
                K720_SensorQuery(MacAddr, StateInfo, RecordInfo)
            }
            if (nRet == 0) {
                var str = ""
                when (StateInfo[0].toInt()) {
                    48 ->{
                        Log.d(TAG, "boxstatus7")

                        str = """${str}Machine Status: Idle """.trimIndent()
                    }
                    49 ->{
                        Log.d(TAG, "boxstatus8")

                        str = """ $str Machine status: card box is full""".trimIndent()
                    }
                    50 ->{
                        Log.d(TAG, "boxstatus9")

                        str = """${str}Machine status: Failed to prepare card, please click "Reset"" """.trimIndent()
                    }
                    52 ->{
                        Log.d(TAG, "boxstatus10")

                        str = """ $str Machine status: command cannot be executed, please click "Reset""""".trimIndent()
                    }
                    56 ->{
                        Log.d(TAG, "boxstatus11")

                        str = """${str}Machine status: Recycle bin is full """.trimIndent()
                    }
                    57 ->{
                        Log.d(TAG, "boxstatus12")

                        str = """${str} Machine status: recycle bin is full/card bin pre-full""".trimIndent()
                    }
                }
                when (StateInfo[1].toInt()) {
                    48 ->{
                        str = """ ${str}Action status: idle  """.trimIndent()
                        Log.d(TAG, "boxstatus11")

                    }
                    49 ->{
                        Log.d(TAG, "boxstatus12")

                        str = """ ${str}Action status: There is an error in receiving the card, please click "Reset"" """.trimIndent()
                    }
                    50 ->{
                        Log.d(TAG, "boxstatus13")

                        str = """${str}Action status: Card issuance error, please click "Reset""""".trimIndent()
                    }
                    52 ->{
                        Log.d(TAG, "boxstatus14")

                        str = """${str}Action status: receiving card""".trimIndent()
                    }
                    56 ->{
                        Log.d(TAG, "boxstatus15")

                        str = """${str}Action Status: Issuing Cards""".trimIndent()
                    }
                }

                when (StateInfo[2].toInt()) {

                    48 -> {
                        Log.d(TAG, "boxstatus1")
                        str = """$str Card box status: The card box is in a non-preemptive state""".trimIndent()
                    }
                    49 -> {
                        Log.d(TAG, "boxstatus2")
                        str = """$str Card box status: card box pre-empty""".trimIndent()
                    }
                    50 ->{
                        Log.d(TAG, "boxstatus3")

                        str = """$str Card box status: Card jammed """.trimIndent()
                    }
                    52 -> {
                        Log.d(TAG, "boxstatus4")

                        str = """ ${str}Card Box Status: Overlapping Cards""".trimIndent()
                    }
                    56 -> {
                        Log.d(TAG, "boxstatus5")

                        str = """$str Card box status: The card issuing box is full and can no longer be recycled to the issuing box/card box pre-empty""".trimIndent()
                    }
                    57 -> {
                        Log.d(TAG, "boxstatus6")

                        str = """${str}Card box status: The card issuing box is full and can no longer be recycled to the issuing box""".trimIndent()

                    }
                }
                when (StateInfo[3].toInt()) {
                    48 -> {
                        Log.d(TAG, "boxstatus")
                        str = """${str}Card Box Status: Idle""".trimIndent()
                        SendBuf[0] = 76
                        SendBuf[1] = 70
                        SendBuf[2] = 3
                        if (Connectflag) {
                            K720_SendCmd(MacAddr, SendBuf, 2, RecordInfo)

                        } else {
                            k720_usb!!.K720_SendCmd(MacAddr, SendBuf, 2)

                        }
                    }
                    49 -> {
                        Log.d(TAG, "stuck in the position of sensor 1 card pickup posi")
                        str = """$str Card box status: stuck in the sensor 1 position (card pickup position""".trimIndent()
                        Log.d(TAG, "getStatus"+type)
                        SendBuf[0] = 76
                        SendBuf[1] = 80
                        SendBuf[2] = 3
                        if (Connectflag){
                            K720_SendCmd(MacAddr, SendBuf, 3, RecordInfo)
                        } else {
                            k720_usb!!.K720_SendCmd(MacAddr, SendBuf, 3)

                        }
                    }
                    50 -> {
                        str = """$str Card box status: stuck in sensor 2 position""".trimIndent()
                        Log.d(TAG, "stuck in the position of sensor 2 card")
                        SendBuf[0] = 76
                        SendBuf[1] = 80
                        SendBuf[2] = 0
                        if (Connectflag){
                            K720_SendCmd(MacAddr, SendBuf, 3, RecordInfo)

                        } else {
                            k720_usb!!.K720_SendCmd(MacAddr, SendBuf, 3)
                        }
                    }
                    51 ->{
                        Log.d(TAG, "stuck in the position of sensor 1-2 card reading posi")
                        str = "${str}Card box status: stuck in sensor 1-2 position (card reading posi".trimIndent()
                        if(type=="CONTRACTOR"){
                            verifyPassword(context,type)
                        }else{

                        }
                        SendBuf[0] = 76
                        SendBuf[1] = 80
                        SendBuf[2] = 0
                        if (Connectflag){
                            K720_SendCmd(MacAddr, SendBuf, 3, RecordInfo)

                        } else {
                            k720_usb!!.K720_SendCmd(MacAddr, SendBuf, 3)
                        }
                    }
                    52 -> {
                        str = """ ${str}Card status: stuck in sensor 3 position""".trimIndent()
                        Log.d(TAG, "stuck in the position 3")
                    }
                    53 -> {
                        str = "$str Card status: stuck at the sensor pick-up position".trimIndent()

                        Log.d(TAG, "stuck in the position of sensor PICK-UP")

                        SendBuf[0] = 76
                        SendBuf[1] = 80
                        SendBuf[2] = 3
                        if (Connectflag) {
                            K720_SendCmd(MacAddr, SendBuf, 3, RecordInfo)

                        } else {
                            k720_usb!!.K720_SendCmd(MacAddr, SendBuf, 3)
                        }
                    }
                    54 ->{
                        str = """${str}Card status: stuck in the position of sensor 2-3""".trimIndent()
                        Log.d(TAG, "stuck in the position of sensor 2-3")
                        SendBuf[0] = 76
                        SendBuf[1] = 80
                        SendBuf[2] = 0
                        if (Connectflag) {
                            K720_SendCmd(MacAddr, SendBuf, 3, RecordInfo)

                        } else {
                            k720_usb!!.K720_SendCmd(MacAddr, SendBuf, 3)
                        }
                    }
                    55 -> { str = """$str Card status: stuck in the position of sensor 1-2-3""".trimIndent()
                        Log.d(TAG, "stuck in the position of sensor 1-2-3")
                        SendBuf[0] = 76
                        SendBuf[1] = 80
                        SendBuf[2] = 0
                        if (Connectflag){
                            K720_SendCmd(MacAddr, SendBuf, 3, RecordInfo)

                        } else {
                            k720_usb!!.K720_SendCmd(MacAddr, SendBuf, 3)
                        }
                    }
                    56 -> {
                        Log.d(TAG, "getStatus: EMPTY")

                        str = """$str Card Status: Card box is empty""".trimIndent()
                    }
                    57 ->{
                        str = """$str Card Status: Only one card is in the sensor 1 position""".trimIndent()
                        Log.d(TAG, "getStatus: sensor 1 position")
                        SendBuf[0] = 76
                        SendBuf[1] = 80
                        SendBuf[2] = 3
                        if (Connectflag) {
                            K720_SendCmd(MacAddr, SendBuf, 3, RecordInfo)
                        } else {
                            k720_usb!!.K720_SendCmd(MacAddr, SendBuf, 3)
                        }
                    }
                    59 -> {
                        Log.d(TAG, "getStatus: sensor 1-2 position")
                        str = """$str Card Status: Only one card is in the sensor 1-2 position""".trimIndent()
                        SendBuf[0] = 76
                        SendBuf[1] = 80
                        SendBuf[2] = 0
                        if (Connectflag){
                            K720_SendCmd(MacAddr, SendBuf, 3, RecordInfo)

                        } else {
                            k720_usb!!.K720_SendCmd(MacAddr, SendBuf, 3)
                        }
                    }
                    62 ->{
                        Log.d(TAG, "getStatus: sensor 2-3 position")
                        str = """$str Card Status: Only one card is in the sensor 2-3 position\r""".trimIndent()
                        SendBuf[0] = 76
                        SendBuf[1] = 80
                        SendBuf[2] = 0
                        if (Connectflag) {
                            K720_SendCmd(MacAddr, SendBuf, 3, RecordInfo)

                        } else {
                            k720_usb!!.K720_SendCmd(MacAddr, SendBuf, 3)
                        }
                    }
                }
                Log.d(TAG, "onClick: $str")
                // ShowMessage(str,context)
            } else {
                // ShowMessage("Sensor status query failed with error code:" + ErrorCode(nRet, 0),context)
            }
        }


In this unit, you will learn to apply anatomical terminology and the concept of levels of organisation when describing the human body and its systems. You will describe the anatomical features, function and physiological regulation of the musculoskeletal, cardiovascular, lymphatic, digestive, respiratory, nervous, endocrine, urinary, and reproductive human body systems. In addition, you will study the anatomical and physiological relations involved in human movement including the effects of use, disuse and ageing on the pelvic region, perineum and lower limbs.
This unit is for students from these courses only: CB66 - Bachelor of Health Science (Allied Health), CB84 - Bachelor of Occupational Therapy (Honours), CB85 - Bachelor of Physiotherapy (Honours), CB86 - Bachelor of Podiatry (Honours), CB87 - Bachelor of Speech Pathology (Honours).