text:
The curator of the Tate Britain Elena Crippa talks about the School of London
Art, Exhibitions
The opening of the exhibition "Francis Bacon, Lucian Freud, and the School of London" at Pushkin State Museum in Moscow gave me a brilliant opportunity to interview curator of Modern and Contemporary British Art at the Tate Britain Elena Crippa about the School of London. The artists of this group are highly demanded in the art market.
This term – "School of London" – adopted by R. B. Kitaj in 1976 to refer to the many outstanding artists based in London who drew and painted the human figure – has often been applied to a small group of six painters: Frank Auerbach, Francis Bacon, R. B. Kitaj, Leon Kossoff, Lucian Freud, and Michael Andrews.
Did the London school have a manifesto and ideas in common, like the artistic group of the past, such as, for example, the "Wanderers" in Russia? Why, in the era of domination of abstract and conceptual art, did the School of London return to figurative painting?
The artists of School of London as well as their teachers David Bomberg and William Coldstream wanted to regain a sense of the stronger attachement to the reality. Possibly, the abstraction is gone too far and became too subjective. They wanted to root back the attention into individuals and situations that were really enclosed them. Bomberg and Coldstream started to draw a painting from life. They painted the friends and relatives alongside with landscapes and cityscapes that were in their area where they lived. They became very important teachers of the reality that became again very strong following the postwar existential period. Francis Bacon was a leading figure who captured the vitality and the struggle of the human existence. I would say that all the artists and the exhibition are very much linked to the historical moment by their drive, the sense of the responding to the urgency of the trauma, by the desire to pin down reality and make it felt and recreated in a very intensified way. For example, in this picture there is a desire to overcome the reality and struggle (R. B. Kitaj "The Wedding", 1989-1993).
R.B. Kitaj (1932-2007)
"The Wedding" 1989-1993
Presented by the artist 1993
© Tate, London, 2019. © The estate of R. B. Kitaj
Each artist is developping his own particular painting style. They are united by the desire to paint something that is very close and intimate to them in the way that not just representing it but in the way to recreate it giving them the sense of the physical presence. The way to achieve this result was also very personal.
Could you tell more about their style?
For example, in Frank Auerbach's painting "To the studios" (1990-1991) there is always the sense of really close structuring and something solid, a sort of dramatical implant. If you look at the building in this particular painting, you would have a feeling to being immersed into the matter of this buildings. Leon Kossof's paintings are more about the mouvement. He has always very clear, bright and shining colors alongside with very energetic brushwork. Some of the painters were using the impasto technique. They all have different artistic style. They painted also the different subjects that they were surrounded.
Frank Auerbach (born 1931)
"To the Studios" 1990-1991
© Tate
© Frank Auerbach
Leon Kossoff (born 1926)
"Christ Church, Spitalfields, Morning" 1990
© Leon Kossoff
Which relationships does the School of London have with the great masters of the past?
If you look at specific painting, you'll recognize Picasso, Cézanne, Chagall, etc. Kitaj said when he painted "The Wedding", he was thinking about Picasso "Les Demoiselles d'Avignon". The human body expresses the vitality of life. Bacon started painting his grotesque figures looking at Picasso's work of 1919-1921. This forms are very synthetic. In Paula Rego work (an artist of late generation of the School of London) you can see a lot from Goya, particularly, in her "Dance", 1988. You can see at some portraits the influence of Rembrandt who was hugely important to many of them.
Paula Rego born 1935
"The Dance" 1988 Purchased 1989
© Paula Rego
You may know Russian artist David Burliuk. He reminded me some of Francis Bacon's work. Do you think if Bacon could be aware of Burliuk's work?
It is a good question. We don't know of this connection. The only Russian connection that we know it came of filmmaker Sergei Eisenstein. Bacon used a lot of films from him. They may be connected by the knowledge of Picasso work or some friends in common.
Francis Bacon (1909-1992)
"Portrait of Isabel Rawsthorne" 1966
© Estate of Francis Bacon
In cooperation with the Tate (London), the Pushkin State Museum presents the exhibition "Francis Bacon, Lucian Freud, and the School of London" in Moscow until 19 May 2019. For the first time, the Russian public will have the chance to get acquainted with a unique and very important chapter in the history of modern British art and explore the legacy of artists who used figurative painting to express their deeply personal, sensual and intense life experience. The exposition includes 80 paintings and graphical artworks from the Tate. VTB Bank is the general sponsor of the exhibition.
Dany Atrache Spring/Summer 2019 show at Paris Haute Couture fashion week
Advices from art advisor Jean-Paul Claverie


Her Hollywood-Optioned Book Is Now in Paperback!
During this year, I've done posts about Allison Winn Scotch's (C'95) book The Time of My Life and how it was optioned by the Weinstein Brothers, was reviewed in People Magazine, made The Today Show's top 10 books for the fall, and made the New York Times Best Seller List! (#31).
Now news that last week, her book came out in paperback!


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text:
\section{Introduction}

Fundamental problems related to the primordial universe or black holes, for example, require a conciliation between quantum mechanics and general relativity, i.e., a quantum description of gravity. String theory \cite{polchinski} is one of the main candidates to provide such quantum description for gravity. However Ho\v{r}ava-Lifhitz (HL) theory of gravity has gained attention in recent years \cite{Horava:2009uw} since it provides a theoretical framework to study quantum gravity in a self contained manner in (3+1) space time dimensions.

Ho\v{r}ava proposed a new model for quantum gravity \cite{Horava:2009uw} based on an anisotropy between space and time. Such anisotropy breaks, therefore, the Lorentz symmetry and it is very common in condensed matter systems \cite{Lifshitz, Lifshitz2, Sachdev}. The model is built in order to be compatible with the anisotropic scaling,
\begin{equation}
    \vec{x}\rightarrow b\vec{x},\,\,\,\,\,t\rightarrow b^z t,
\end{equation}
where the parameter $z$ which controls the degree of anisotropy is called critical exponent. The anisotropic scaling reflects on the mass dimensions of all fields, operators and coupling constants, so that,
\begin{equation}
    [\vec{x}]=-1,\,\,\,\,\,[t]=-z.
\end{equation}
The great interest in HL model for gravity lies in the fact that the gravity becomes power counting renormalizable when $z=3$, since the dimension of the gravitational coupling constant goes to zero. After Ho\v{r}ava's seminal paper \cite{Horava:2009uw}, several studies were done within the context of gravity \cite{DOdorico:2015pil, Lopes:2015bra, Hartong:2016yrf, Hartong:2015zia}, black holes \cite{Wei:2019zdf, Xu:2018tdh, Xu:2020xsl, AyonBeato:2009nh}, cosmology \cite{Kiritsis:2009sh, Calcagni:2009ar, Oliveira-Neto:2019tvo, Pitelli:2012sj}, holography \cite{Griffin:2012qx, Christensen:2013lma, Mohammadi:2020jbe} and so on.

More recently other HL-like field theories were constructed. Extensions of QED with lifshitz scaling were studied specially in the context of radiative corrections and renormalization \cite{Gomes:2018umk, Gomes:2016ixw}. HL-like extensions for Gross-Neveu \cite{Lima:2016qgr} and four-fermions \cite{Gomes:2020nbz, Mariz:2019kmc, Mariz:2019iij} models were also studied. The finite temperature effects were studied in HL-like extensions of the scalar QED and for Yukawa coupling \cite{Farias:2013rya}.

A Bose-Einstein condensation (BEC) \cite{Einstein} occurs when a low density gas of bosons is cooled to temperatures near to zero kelvin. Under such conditions a considerable portion of the bosons fall into the lowest quantum state, forming therefore a single collective quantum wave called Bose-Einstein condensate \cite{Huang}. After the first Bose-Einstein condensates produced with rubidium \cite{Anderson} and sodium atoms \cite{Davis}, several studies were carried out in the context quasi-particles \cite{Deng, Kasprzak, Balili, Demokritov}, photons gases \cite{Klaers1} and molecules \cite{Klaers2}.

Bose-Einstein condensates has been intensively studied in the context of high energy physics as well. The critical temperature of Bose-Einstein condensation in Rindler space has been analyzed in \cite{Takeuchi:2015nga}. The effects of Lorentz symmetry violation in the BEC were studied in \cite{Furtado:2020olp, Casana:2011bv, deSales:2011jy, Castellanos:2010zz, Colladay:2006rt}. Also brane-world scenarios \cite{Casadio:2016aum, Kasamatsu:2013lda}, cosmology \cite{Erdem:2019gpk, Atazadeh:2016zls} and black holes \cite{Garay:1999sk, Kuhnel:2015qaa} were analyzed in connection with BEC.

In this paper we study the corrections emergent from a Ho\v{r}ava-Lifshitz extension of the complex scalar sector to BEC and to the thermodynamics parameters. We initially discussed some features of the model to only then compute the corrections to the BEC. The calculations were done by computing the generating functional, from which we extract the thermodynamics parameters. We also obtained the Lifshitz scaling correction for the critical temperature $T_c$ that sets the Bose-Einstein condensation.

This paper is organized as follows: in the next section we present the model itself and we compute the thermodynamic parameters, such as pressure, energy, specific heat and charge density when $z=2$, which is the simplest non-trivial case. In section III we extend the calculations of the section II for the case of a generic $z$. We also calculate the critical temperature for the BEC. In section IV we present our final remarks.

\section{Case $z=2$}\label{casez2}
The model we are considering consists of the Ho\v{r}ava-Lifshitz extension of the scalar sector with critical exponent $z=2$. Hence the lagrangian describing the system is

\begin{eqnarray}\label{lagrangian1}
\mathcal{L}&=&\partial_0\phi(\partial_0\phi)^*-\partial_i\partial_j\phi(\partial_i\partial_j\phi)^*-m^4\phi\phi^*.
\end{eqnarray}
In the present model the lagrangian has mass dimension $d=5$ and the mass dimension of the parameters are the following:
\begin{eqnarray}\label{massdimensions}
[\phi]=\frac{1}{2},\,\,[m]=1.
\end{eqnarray}

The lagrangian (\ref{lagrangian1}) possess an obvious $U(1)$ symmetry, so that
\begin{equation}
    \phi\rightarrow \phi'=e^{-i\alpha}\phi,
\end{equation}
with $\alpha\in\mathbb{R}$. The Noether's theorem states that for any given continuous symmetry there is a conserved quantity in connection. In order to find such conserved quantity let us consider $\alpha=\alpha(x)$, i.e., a function of spacetime position, so that the Euler-Lagrange equation gives us the equation of motion for the ``field'' $\alpha(x)$. Since the contribution $\partial\mathcal{L}/\partial\alpha=0$, we can find the following conserved current,
\begin{equation}
    j_{k}(x)=i\left(\partial_m\phi\partial_m\partial_k\phi^*-\partial_m\partial_k\phi\partial_m\phi^*+\phi^*\partial_k\partial_m^2\phi-\phi\partial_k\partial_m^2\phi^*\right),
\end{equation}
and charge density
\begin{eqnarray}
    \nonumber Q&=&\int d^3x j^0\\
    &=&\int d^3x\left[i\left(\phi^*\frac{\partial\phi}{\partial t}-\phi\frac{\partial\phi^*}{\partial t}\right)\right].
\end{eqnarray}

Making use of the equations of motion for $\phi$ and $\phi^*$, given by
\begin{eqnarray}
-\partial_0^2\phi-\partial_m^2\partial_n^2\phi-m^4\phi&=&0\\
-\partial_0^2\phi^*-\partial_m^2\partial_n^2\phi^*-m^4\phi^*&=&0,
\end{eqnarray}
a straightforward calculation shows us the conservation of the four current, i.e., $\partial_{\mu}j^{\mu}(x)=0$. Splitting the fieds $\phi$ and $\phi^*$ into two real components $\phi_1$ and $\phi_2$ as
\begin{eqnarray}
    \phi&=&\frac{1}{\sqrt{2}}(\phi_1+i\phi_2)\\
    \phi^*&=&\frac{1}{\sqrt{2}}(\phi_1-i\phi_2),
\end{eqnarray}
we can rewrite the Lagrangian in terms of $\phi_a$ with $a=1,2$ as follows
\begin{eqnarray}
    \mathcal{L}&=&\frac{1}{2}\partial_{0}\phi_a\partial_{0}\phi_a-\frac{1}{2}\partial_{i}\partial_{j}\phi_a\partial_{i}\partial_{j}\phi_a-\frac{m^4}{2}\phi_a\phi_a.
\end{eqnarray}
The canonically conjugated momenta are:
\begin{eqnarray}\label{momenta}
    \pi_a=\partial_0\phi_a
\end{eqnarray}
then the Hamiltonian becomes
\begin{eqnarray}
    \mathcal{H}=\frac{1}{2}\left(\pi_a\pi_a+\partial_{i}\partial_{j}\phi_a\partial_{i}\partial_{j}\phi_a+m^4\phi_a\phi_a\right).
\end{eqnarray}
The charge density can also be expressed in terms of $\phi_a$,
\begin{equation}\label{chargedensity1}
    Q=\int d^3x\epsilon_{ab}\pi_a\phi_b.
\end{equation}
Letting $\mathcal{H}(\phi,\pi)\rightarrow\mathcal{H}(\phi,\pi)-\mu\mathcal{N}(\phi,\pi)$, where $\mathcal{N}(\phi,\pi)$ is the conserved charge density, identified as $Q$, and $\mu$ is the chemical potential, the partition function becomes:
\begin{eqnarray}\label{Z1}
    \nonumber Z&=&\int D\pi_a\int_{periodic}D\phi_a\exp\left\{\int_0^{\beta}d\tau\int d^3x\times\right.\\
    &&\times\left.\left[i\pi_a\frac{\partial\phi_a}{\partial\tau}-\mathcal{H}(\phi_a,\pi_a)+\mu\epsilon_{ab}\pi_a\phi_b\right]\right\}.
\end{eqnarray}
Note that the $[\mu]=2$. The term ``periodic'' states for the fact that the integration over the field is constrained in such way that $\phi(\vec{x},0)=\phi(\vec{x},\beta)$ with $\beta=1/T$. The partition function can be written as
\begin{eqnarray}\label{Z2}
    \nonumber Z&=&\int D\pi_a\int_{periodic}D\phi_a\exp\left\{\int_0^{\beta}d\tau\int d^3x\times\right.\\
    \nonumber&&\times\left.\left[-\frac{1}{2}\pi_a^2+\left(i\frac{\partial\phi_a}{\partial\tau}-\mu\epsilon_{ab}\phi_b\right)\pi_a\right.\right.\\
    &&\left.\left.-\frac{1}{2}\partial_{i}\partial_{j}\phi_a\partial_{i}\partial_{j}\phi_a-\frac{1}{2}m^4\phi_a^2\right]\right\}.
\end{eqnarray}

The integration over the momenta can be directly done. Then we obtain,
\begin{eqnarray}\label{Z3}
    \nonumber Z&=&(N')^2\int_{periodic}D\phi_i\exp\left\{\int_0^{\beta}d\tau\int d^3x\times\right.\\
    \nonumber&&\times\left.\left[\frac{1}{2}\left(i\frac{\partial\phi_b}{\partial\tau}-\mu\epsilon_{ab}\phi_a\right)^2-\frac{1}{2}\partial_{i}\partial_{j}\phi_a\partial_{i}\partial_{j}\phi_a-\frac{1}{2}m^4\phi_a^2\right]\right\}.\\
\end{eqnarray}
The factor $N'$ is an irrelevant normalization constant, since multiplication of $Z$ by any constant does not change the thermodynamics. The components of $\phi$ can be Fourier-expanded as,
\begin{eqnarray}\label{Fourier}
    \phi_1&=&\sqrt{2}\zeta\cos\theta+\sqrt{\frac{\beta}{V}}\sum_{n}\sum_{\vec{p}}e^{i(\vec{p}\cdot\vec{x}+\omega_n\tau)}\phi_{1;n}(\vec{p})\\
    \phi_2&=&\sqrt{2}\zeta\sin\theta+\sqrt{\frac{\beta}{V}}\sum_{n}\sum_{\vec{p}}e^{i(\vec{p}\cdot\vec{x}+\omega_n\tau)}\phi_{2;n}(\vec{p}),
\end{eqnarray}
where $\omega_n=2\pi n T$, owing to the constraint of periodicity that $\phi(\vec{x},\beta)=\phi(\vec{x},0)$ for all $\vec{x}$. Here $\zeta$ and $\theta$ are independent of spacetime position and determine the full infrared behaviour of the field; that is, $\phi_{1;0}(\vec{p}=\vec{0})=\phi_{1;0}(\vec{p}=\vec{0})=0$. This allows for the possibility of condensation of the bosons into the zero-momentum state. Substituting (\ref{Fourier}) into (\ref{Z2}) the partition function becomes
\begin{equation}
    Z=(N')^2\prod_n\prod_p\int D\phi_{1;n}(\vec{p})D\phi_{2;n}(\vec{p})e^{S},
\end{equation}
where $S$ is given by

\begin{eqnarray}
    \nonumber S&=&\beta V(\mu^2-m^4)\zeta^2\\
    &&-\frac{1}{2}\sum_n\sum_p\left(\phi_{1;-n}(-\vec{p}),\phi_{2;-n}(-\vec{p})\right)D\left(\begin{array}{c}
\phi_{1;n}(\vec{p})   \\
\phi_{1;n}(\vec{p})
    \end{array}\right),
\end{eqnarray}
being $D$

\begin{eqnarray}
    D=\beta^2\left(\begin{array}{cc}
    \omega_n^2+\omega^2-\mu^2 & -2\mu\omega_n \\
    2\mu\omega_n & \omega_n^2+\omega^2-\mu^2
    \end{array}\right),
\end{eqnarray}
with $\omega=\sqrt{\vec{p}^4+m^4}$. Carrying out the integrations over $\phi_{1;n}$ and $\phi_{2;n}$, we have,
\begin{equation}
    \ln Z=\beta V(\mu^2-m^4)\zeta^2+\ln (\det D)^{-1/2},
\end{equation}
so that we can rewritte in the following form

\begin{eqnarray}\label{generatingfunctional}
    \nonumber\ln Z&=&\beta V(\mu^2-m^4)\zeta^2\\
    \nonumber&&-V\int\frac{d^3p}{(2\pi)^3}\left\{\beta\omega+\ln\left[1-e^{-\beta(\omega-\mu)}\right]+\ln\left[1-e^{-\beta(\omega+\mu)}\right]\right\}\\
\end{eqnarray}

It is important to highlight here that the above expression for $\ln Z$ was obtained under the consideration of the following convergence condition
\begin{equation}\label{convergence}
    \left|\mu\right|\leq m^2.
\end{equation}
A modification of the usual convergence condition ($|\mu|\leq m$) already known in the literature, first stated in the work of Haber \cite{Haber:1981fg}.
The usual relation
\begin{equation}
    \frac{PV}{T}=\ln Z,
\end{equation}
gives us the equation of state for the system. Hence the pressure is given by
\begin{eqnarray}\label{pressurecomplete}
    \nonumber P&=&(\mu^2-m^4)\zeta^2\\
    \nonumber&&-\frac{1}{\beta}\int\frac{d^3p}{(2\pi)^3}\left\{\beta\omega+\ln\left[1-e^{-\beta(\omega-\mu)}\right]+\ln\left[1-e^{-\beta(\omega+\mu)}\right]\right\}.\\
\end{eqnarray}
The internal energy can be written as
\begin{eqnarray}\label{energy}
    \nonumber E&=&-\frac{\partial}{\partial \beta}\ln Z\\
   \nonumber &=&-V(\mu^2-m^4)\zeta^2\\
    &&-V\int\frac{d^3p}{(2\pi)^3}\left\{-\omega+\frac{-\mu-\omega}{e^{\beta(\mu+\omega)}-1}-\frac{\mu-\omega}{e^{\beta(\omega-\mu)}-1}\right\}.
\end{eqnarray}
The specific heat at constant volume is expressed by

\begin{eqnarray}\label{heat}
    \nonumber C_v&=&\frac{\partial E}{\partial T}\\
    \nonumber&=&-V\beta^2\int\frac{d^3p}{(2\pi)^3}\left\{\frac{(\mu-\omega)(\omega-\mu)e^{-\beta(\omega-\mu)}}{1-e^{-\beta(\omega-\mu)}}\right.\\
    \nonumber&&+\left.\frac{(\mu-\omega)(\omega-\mu)e^{-2\beta(\omega-\mu)}}{\left(1-e^{-\beta(\omega-\mu)}\right)^2}\right.\\
    \nonumber&&+\frac{(-\mu-\omega)(\omega+\mu)e^{-\beta(\omega+\mu)}}{1-e^{-\beta(\omega+\mu)}}\\
    &&+\left.\frac{(-\mu-\omega)(\omega+\mu)e^{-2\beta(\omega+\mu)}}{\left(1-e^{-\beta(\omega+\mu)}\right)^2}\right\}
\end{eqnarray}
The charge density is written as

\begin{eqnarray}\label{charge}
    \nonumber\rho&=&\frac{1}{\beta V}\frac{\partial \ln Z}{\partial \mu}\\
     &=& 2\mu\zeta^2+\int\frac{d^3p}{(2\pi)^3}\left[\frac{e^{-\beta  (\omega -\mu )}}{1-e^{-\beta  (\omega -\mu )}}-\frac{e^{-\beta  (\mu +\omega )}}{1-e^{-\beta  (\mu +\omega )}}\right]
\end{eqnarray}
Using spherical coordinates, the integration measure goes to

\begin{equation}
    \int\frac{d^3p}{(2\pi)^3}\longrightarrow\frac{1}{2\pi^2}\int dp p^2.
\end{equation}
In a non-condensate fase, by setting $\zeta=0$, the expressions for the above thermodynamic quantities can be simplified. So that we obtain for the pressure

\begin{eqnarray}\label{pressurecomplete1}
    \nonumber P=-\frac{1}{\beta}\frac{1}{2\pi^2}\int dp p^2\left\{\beta\omega+\ln\left[1-e^{-\beta(\omega-\mu)}\right]+\ln\left[1-e^{-\beta(\omega+\mu)}\right]\right\},\\
\end{eqnarray}
for the energy
\begin{eqnarray}\label{energy2}
     E=-V\frac{1}{2\pi^2}\int dp p^2\left\{-\omega+\frac{-\mu-\omega}{e^{\beta(\mu+\omega)}-1}-\frac{\mu-\omega}{e^{\beta(\omega-\mu)}-1}\right\},
\end{eqnarray}
for the specific heat at constant volume
\begin{eqnarray}\label{heat2}
    \nonumber C_v&=&-V\beta^2\frac{1}{2\pi^2}\int dp p^2\left\{\frac{(\mu-\omega)(\omega-\mu)e^{-\beta(\omega-\mu)}}{1-e^{-\beta(\omega-\mu)}}\right.\\
    \nonumber&&+\left.\frac{(\mu-\omega)(\omega-\mu)e^{-2\beta(\omega-\mu)}}{\left(1-e^{-\beta(\omega-\mu)}\right)^2}\right.\\
    \nonumber&&+\frac{(-\mu-\omega)(\omega+\mu)e^{-\beta(\omega+\mu)}}{1-e^{-\beta(\omega+\mu)}}\\
    &&+\left.\frac{(-\mu-\omega)(\omega+\mu)e^{-2\beta(\omega+\mu)}}{\left(1-e^{-\beta(\omega+\mu)}\right)^2}\right\},
\end{eqnarray}
and finally for the charge density
\begin{eqnarray}\label{charge2}
    \rho&=&\frac{1}{2\pi^2}\int dp p^2\left[\frac{e^{-\beta  (\omega -\mu )}}{1-e^{-\beta  (\omega -\mu )}}-\frac{e^{-\beta  (\mu +\omega )}}{1-e^{-\beta  (\mu +\omega )}}\right].
\end{eqnarray}

At this point it is important to discuss the influence of the critical exponent $z=2$ in the critical temperature $T_c$ that sets the Bose-Einstein condensation. For the occurrence of the Bose-Einstein condensation we must have $\mu=\pm m^2$. Applying such condition in (\ref{charge2}) we obtain
\begin{equation}
    T_c=\sqrt{\frac{3\rho}{m^2}},
\end{equation}
which is the correction for the critical temperature first presented in \cite{Haber:1981fg}.

\section{Arbitrary $z$ case}

For a generic critical exponent $z$ we have the following lagrangian.

\begin{eqnarray}\label{lagrangianz}
\mathcal{L}=\partial_0\phi(\partial_0\phi)^*-\partial_{i1}\partial_{i2}\cdots\partial_{iz}\phi(\partial_{i1}\partial_{i1}\cdots\partial_{iz}\phi)^*-m^{2z}\phi\phi^*.
\end{eqnarray}
The mass dimension of the lagrangian is $d+z$ being $d$ the spatial dimension which in our work is considered as $d=3$. In this case the spatial derivative has dimension $[\partial_i]=1$ while the temporal derivative has dimension $[\partial_0]=z$. The mass dimension of the scalar field and the mass parameter are the same as presented in (\ref{massdimensions}).

\begin{figure*}[ht!]
    \centering
    \includegraphics[scale=0.6]{rho_x_b.eps}
    \caption{Charge density for $z=1$, $z=2$ and $z=3$. In this plot we have considered $\mu=1$ and $m=2$.}
    \label{fig1}
\end{figure*}

The same procedure employed in section (\ref{casez2}) can be applied here so that we can found the Hamiltonian density as:
\begin{eqnarray}
    \mathcal{H}=\frac{1}{2}\left(\pi_a\pi_a+\partial_{i1}\partial_{i2}\cdots\partial_{iz}\phi_a\partial_{i1}\partial_{i2}\cdots\partial_{iz}\phi_a+m^{2z}\phi_a\phi_a\right).
\end{eqnarray}
The charge density and the momenta are kept unchanged, i.e., they are given by (\ref{momenta}) and (\ref{chargedensity1}). Thence the generating functional can be written as follows

\begin{eqnarray}\label{Zz}
    \nonumber Z&=&\int D\pi_a\int_{periodic}D\phi_a\exp\left\{\int_0^{\beta}d\tau\int d^3x\times\right.\\
    \nonumber&&\times\left.\left[-\frac{1}{2}\pi_a^2+\left(i\frac{\partial\phi_a}{\partial\tau}-\mu\epsilon_{ab}\phi_b\right)\pi_a\right.\right.\\
    &&\left.\left.-\frac{1}{2}\partial_{i1}\partial_{i2}\cdots\partial_{iz}\phi_a\partial_{i1}\partial_{i2}\cdots\partial_{iz}\phi_a-\frac{1}{2}m^{2z}\phi_a^2\right]\right\}.
\end{eqnarray}
The chemical potential for the generic $z$ case has mass dimension $[\mu]=z$. The final form of the partition function after the integrations and the sum over the Matsubara frequencies is same as presented in (\ref{generatingfunctional}), where the only differences are the expression for the dispersion relation, which is given by $\omega=\sqrt{\vec{p}^{2z}+m^{2z}}$ and the term related to the condensed fase $\beta V(\mu^2-m^{2z})\zeta^2$. Consequently, the expressions for the pressure, energy, specific heat and charge density in the non-condensate fase are also the same as those presented in equations (\ref{pressurecomplete1}), (\ref{energy2}), (\ref{heat2}) and (\ref{charge2}) respectively.

The convergence condition is also modified by the critical exponent $z$. For a generic $z$ we have the following convergence condition
\begin{equation}\label{convergenceZ}
    |\mu|\leq m^{z},
\end{equation}
which restores the usual convergence criteria first stated by Haber \cite{Haber:1981fg} when $z=1$. From this corrected convergence criteria we can obtain, with the same procedure used in the previous section, the critical temperature for an arbitrary critical exponent $z$. Therefore from (\ref{convergenceZ}) we obtain
\begin{equation}\label{Tcz}
    T_c=\sqrt{\frac{3\rho}{m^z}}.
\end{equation}
As we can see from (\ref{Tcz}), as we increase the critical exponent the critical temperature for the Bose-Einstein condensation decreases.

We plot the qualitative behaviour of the charge density (fig. \ref{fig1}) and specific heat at constant volume (fig. \ref{fig2}) for three values of the critical exponent $z$, namely, $z=1$, $z=2$ and $z=3$. We have considered for this plot the chemical potential $\mu=1$ and $m=2$. As we can see for both charge density and specific heat, the increasing of $z$ turns the divergence around $\beta=0$ softer. Also when $\beta\rightarrow \infty$ ($T\rightarrow 0$) the effect of $z$ becomes negligible.

\begin{figure*}[ht!]
    \centering
    \includegraphics[scale=0.6]{calor_x_b.eps}
    \caption{Specific heat for volume unit for $z=1$, $z=2$ and $z=3$. In this plot we have considered $\mu=1$ and $m=2$.}
    \label{fig2}
\end{figure*}

\section{Final Remarks}

In this paper we study the corrections emergent from a Ho\v{r}ava-Lifshitz extension of the complex scalar sector to the Bose-Einstein condensation and to the thermodynamics parameters. We initially discussed some features of the model to only then compute the corrections to the Bose-Einstein condensation. The calculations were done by computing the generating functional, from which we extract the thermodynamic parameters. We also obtained the Lifshitz scaling correction for the critical temperature $T_c$ that sets the Bose-Einstein Condensation.

We considered initially the first non-trivial case of critical exponent, i.e., $z=2$. For $z=2$ case we calculate the analytical expressions for pressure, energy, specific heat and charge density. Besides we also obtained a correction for the convergence criteria for the generating functional from which we compute the Bose-Einstein condensation critical temperature.

We also addressed the generic $z$ case, from which we obtain the pressure, energy specific heat and charge density, as well as the Bose-Einstein condensation critical temperature. We could see that increasing the value of $z$ the Bose-Einstein critical temperature decreases. A natural continuation of this work consists in the consideration of self interacting scalar fields.

redpajama_set_name: RedPajamaArXiv


text:
This is a list of electoral results for the electoral district of Norman in Queensland state elections.

Members for Norman

Election results

Elections in the 1960s

Elections in the 1950s

References

Queensland state electoral results by district

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text:
Auto No My Guild
Southern California's Car Dangers
Southern California is one of the most beautiful places to live in the entire United States. The region is home to pristine beaches, beautiful forests, stunning mountains, and thriving cities. Los Angeles is the largest city in California (not to mention the second-largest in the entire nation) and it is surrounded by cities that are metropolitan areas in their own right – such as Long Beach, California. But if there's one thing that Southern California lacks, it's effective mass transit. Because of how spread out the massive population is, Southern California is a place for cars — and that can be a dangerous thing.
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A doctor invents a resurrection formula and tests it by killing his assistant over and over and over again.
Dr. Vick: You are more alive than life itself!
What a surprise this film is! It's a quiet, get-absorbed-in-it sort of horror film, and properly light on gore. The story is similar to Mary Shelley's Frankenstein, whereas life is created from death in the name of science. The acting is solid and moving; there is no mugging, no sly popular culture wink-winks. The focus is on the story, not special effects, not body count, and there's a steady sense of sadness and madness that made me not want to watch the bonus features afterward; I got so drawn into the characters that I did not want their effect on me altered by watching the actors goof around or discuss the film.
The actor who played Adam, the loner medical student, was wonderful -- and very handsome, to boot. He conveyed very well the pain and isolation that Adam felt, and it made sense why Adam would take part in Dr. Vick's experiment for, in part, he'd finally have a connection with another person, regardless of any personal consequences.
Any faults I found with the film were too minor for me to give them much consideration. It's too nice to finally see a low-budget film that obviously was a work of love and is dedicated to its story, not to getting its talent noticed by making yet another indistinguishable gorefest that is a checklist of a dozen other horror films.
And not once does a screeching cat leap out from a closed cupboard door. Mad props for that, guys.


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text:
- a madhouse, a madhouse, I tell ya -
Other alien characters to appear on the series include one Dr Liam Neesam, played by John Cleese. He originally arrives on earth with the intention of destroying it ("because it's blocking our view!") but relents after his encounters with Dick. Not realising that Dick is also an alien, Neesam decides that a species capable of producing a being of such intelligence might just be worth preserving after all.
Neesam returns however in a later episode, this time with the intention, not to destroy humankind, but to transform all human beings into simians, turning Earth into a Planet Monkey World tourist destination in the process. Again Dick foils his plans, on this occasion by using Neesam's own transforming device to turn him (i.e. Neesam) into a chimpanzee.
Unfortunately Mary witnesses the episode leaving Dick wit>h no choice to reveal his true identity to her. Later it transpires that a complaint is lodged against Dick for violation of alien code of conduct - transforming a fellow alien into a chimpanzee - and the Big Giant Head orders the entire crew back to the home planet effectively ending the mission ... and the series.


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MADE WITH ITALIAN LEATHER AND MATCHING LEATHER LINING. MADE IN LOS ANGELES.


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I like the idea's of this, but I get claustrophobic, so I am asking, is the bed raised just to put storage under? or is there another reason the beds are always so high (near the roof lining) in these builds.. this is NOT a criticism, just an open question..
sorry for the probably daft question, but what is Aluminuim Z (I assume its the channel shape, but I have never heard of it, so want to check I am thinking along the correct lines).. question aside, nice job, does it make life easier to find tools, or is it pure cosmetics?
as a former smoker, they regularly fall out of our pockets as we exit our cars.. and often we don't realise until its time to light up, and.. no lighter.. lol..
Thank you, that is what I had assumed was the main reason.
hi, first off, nice one, I have been considering making a similar rough terrain electric vehicle, and was considering Lipo batteries, so I thought I'd ask why you chose lead acid?
I thought there was a "be nice" in your feedback requirement on here.. I did a similar "play" with a ring light by wrapping led (soft white) xmas lights around a small "hulahoop" and shooting through it with a short (13mm) lens.. it worked for what I and the client wanted.. and I got the images required, and both myself and the client were very happy, yes, there are always other ways of doing things, but just because its not the same as "most" people do it, does not make it a bad idea.. can it be improved.. probably, but again, that's for the designer to resolve.. btw I do have proper light rings too, but sometimes you want to stand out from the "crowd" who do it the "normal" way!Also, a rectangle light would change the dynamics a fair bit, and create a very different eye reflection, something that probably would not be quite what Simon wanted.Very nice work Simon.


text:
Daniel Pearson – Lost My Way
Ok, I kinda like this a lot. It's not country, it's not 60's folk rock it's actually some where in between. That makes it a fairly rare gem in my book. Daniel has such an interesting tone and an almost rough edge to his voice. He has a great cadence working for him in this track. It's fun to listen to. I really enjoy the melody in the chorus especially. The guitar line is really well crafted, it's very subdued through most of the song. But it kick up a notch during the chorus. I think I'm going to end up with this little ditty stuck in my head for a while.
I'm curious as to his other songs. I really like the style of this song and I hope some of his other work is in the same style. I would be equally happy to find that he writes and preforms in different song styles. I think it can be a lot of fun to listen to musicians play around with other genre's even if it's just adding an element or two to a song.
Who They Are:
The past few years have seen Leeds-based troubadour Daniel Pearson quietly build a reputation as being one of the best new singer-songwriters around. Blending elements of indie rock, alt.country and classic guitar pop, his immediately accessible songs deliver the emotional connection and honesty that only instinctively great songwriting can provide.
Daniel's soulful vocals and finely-crafted songs have found themselves on the airwaves of BBBC 6Music, BBC Introducing, XFM, Amazing Radio and Australia's biggest radio station Triple J. Writers for Uncut Magazine, Drowned In Sound, Shout 4 Music, Pop Matters, R2 Magazine, AllGigs, Sabotage Times, For Folks Sake and No Depression have been quick to celebrate the arrival of a new voice and have drawn comparisons to Ryan Adams, Bob Dylan and Bruce Springsteen in a series of rave reviews for his two albums Satellites and Mercury State.
Already a veteran of rock n' roll and punk bands by his early-twenties, he had toured up and down the UK and released various singles and EPS before going solo in 2010. After deciding to maintain his artistic independence away from the machinations of a larger label, Daniel has become a very successful example of the new music industry – an artist that maintains control over every aspect of his career, has a real connection with a loyal and growing fanbase and competes for press and radio coverage with acts with huge marketing budgets through the simple strength of his music.
A compelling live performer, Pearson has shared a stage with acts like Michael Kiwanuka, One Night Only, The Bluetones, Willy Mason and Josephine as well as playing a string of headline dates of his own in the UK and USA. In an age of instant stardom, talent shows and endless media hyperbole, he is proving himself as a genuine
Daniel Pearson
Where You Can Get It:
Tags: Country, Folk Rock
All That Crawls / Anders Colsefni – The Endless
Life Lessons – Between You, Me, & Everyone Else


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text:
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    <title>getAuthor</title>
<link href="../../../images/logo-icon.svg" rel="icon" type="image/svg"><link href="../../../styles/style.css" rel="Stylesheet"><link href="../../../styles/logo-styles.css" rel="Stylesheet"><link href="../../../styles/jetbrains-mono.css" rel="Stylesheet"><link href="../../../styles/main.css" rel="Stylesheet">

structureblocklib-root/com.github.shynixn.structureblocklib.api.entity/StructureSaverAbstract/getAuthor

get<wbr></wbr>Author

abstract fun getAuthor(): String
Content copied to clipboard

Gets the author. The author is a optional meta data in the final structure file.

Return

author.

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text:
in: Sword Coast Legends Wiki
Sword Coast Legends
Revision as of 12:05, 25 February 2020 by Encredechine (talk | contribs)
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n-Space
Digital Extremes
Windows, Linux, macOS, PlayStation 4, Xbox One
Roleplaying, Fantasy
Singleplayer, Multiplayer
Rating(s)
USK/PEGI: 16
Sword Coast Legends is a real time adventure game based on Dungeons and Dragons 5th edition. The game includes missions for 1-4 players as well as a dungeon master layout.
Sword Coast Legends is set to become a game which allows players to work through various missions, while allowing players to take part in asymmetric gameplay with a mode where players can challenge each other.
Campaigns and missions are made to fit with the Fantasy RPG setting allowing for more immersive gameplay and more entertaining stories. Players may play solo to work through the campaign without the need for more players where as multiplayer modes are available for those who wish to play with their friends.
The Asymmetric gameplay of having one player play as the Dungeon master against their friends who fight their way through the dungeon. Dungeon masters are able to create the dungeon in whatever way they wish and may place monsters throughout the dungeon for the heroes to fight against. This mode makes sure those who may get bored of playing normally have another method available to them to continue playing.
This game was developed by n-Space, and released on October 20, 2015 by publisher Digital Extremes via Steam.
Sword Coast Legend's YouTube Channel


Here at Crosslink, we want to Impact the Valley. Part of how we do that is proudly partnering with these local heroes in our community! We value the difference they make for the Gospel of Jesus Christ and are thankful for their work in ministry.
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Belong. QL2's Chaos Project for 2018
Every year Canberra's young dancers audition for the Chaos Project staged by QL2. The umbrella name suggests the chaotic situation with which the project begins—in 2018 there were 45 young dancers, boys and girls, aged from eight upwards. But of course by the time the show hits the stage the chaos is gone and, despite the age and experience of the dancers, we the audience are always treated to a wonderful evening of youth dance. The 2018 project, called Belong, had sections choreographed by Olivia Fyfe, Jodie Farrugia and Luke Fryer with Ruth Osborne adding (with her usual flair) an opening and closing section. The topic for exploration—'belonging'—generated some interesting choreographic responses including the addiction (and disconnection from others) to smart phones and social media; supporting others in a variety of ways; bullying; and other similar matters affecting young people. Dance for the times!
Liz Lea and RED
Liz Lea will present her truly exceptional work RED in Liverpool, England, in November as part of the LEAP Festival. It will have a one-off performance on 7 November at 6pm at the Warehouse Studio Theatre, Hope University Creative Campus. RED premiered in Canberra earlier this year. Follow this link for my review of the premiere performance.
Liz Lea in a study for RED, 2018
Sydney Dance Company in 2019
Sydney Dance Company has announced its season program for 2019, which will celebrate what is the company's 50th anniversary. Season choreography will be by Rafael Bonachela, Gabrielle Nankivell, Melanie Lane and Gideon Obarzanek. Full details at this link.
While each of the three programs that will take place over 2019 promises something unusual, it will definitely be fascinating to see what Obarzanek does with a work called Us 50 in which, in the spirit of the anniversary, he will use 50 dancers drawn from former and current company dancers, along with members of the community.
Former and current dancers from Sydney Dance Company: (left to right) Kip Gamblin, Linda Ridgeway, Rafael Bonachela, Sheree Zellner (da Costa), Lea Francis and Bradley Chatfield. Photo: © Pedro Greig
Oral history: Ariette Taylor
My most recent oral history interview for the National Library was with Ariette Taylor, whose contribution to the work of Australian Dance Theatre during the directorship of Jonathan Taylor has probably not been fully explored to date. In addition to a discussion of her work in Adelaide, the interview includes Taylor's background as a dancer in Holland and with Ballet Rambert, and her work as a theatre director after the Taylor family moved from Adelaide to Melbourne.
Remi Wortmeyer
As part of my research for the interview with Ariette Taylor I was searching for information about Mascha ter Weeme, who directed Ballet der Lage Landen, which Taylor joined in Amsterdam in 1957. I accidentally came across some news about Remi Wortmeyer, former dancer with the Australian Ballet and now principal with the Dutch National Ballet. This is old news (from 2016) but I had not come across it before so am posting it here in case any of my readers have also not heard it.
Wortmeyer was, in 2016, the recipient of the beautifully named Mr Expressivity Award at the international ballet festival, Dance Open, in St Petersburg. The trophy, I understand, replicates the lower leg of Anna Pavlova!
Wortmeyer's website is at this link and the images above are from this site.
Jacob's Pillow (again)
The latest post from Jacob's Pillow is a series of video clips with the links between the clips centring on black costuming. There is a clip of David Hallberg dancing Nacho Duato's solo Kaburias, which makes me think back to that wonderful piece, Por vos muero, which was at one stage in the repertoire of the Australian Ballet but not seen for a number of years now. For my New Zealand readers there is a short clip of an early piece by Black Grace, Minoi, seen at the Pillow in 2004. Then there is a mesmerising clip from Un ballo, a work choreographed by Françoise Adret,with perhaps a nod to Duato, for Lyon Opera Ballet. Lots more. Check out the Pillow's dance interactive site .
Meryl Tankard's Two Feet
I have long regretted that Meryl Tankard's solo show Two Feet has never been revived. Well news just in from the Adelaide Festival 2019 is that Tankard is reviving the work for next year's festival. It will feature the remarkable Natalia Osipova. I imagine tickets will fly out the door!
Press for October 2018
'Bravissimo bringing ballet gala to town.' Preview of World Superstars of Ballet Gala, Bravissimo Productions. The Canberra Times, 1 October 2018, p. 20. Online version
'Uneven but often impressive show.' Review of Happiness is …, Canberra Dance Theatre. The Canberra Times, 16 October 2018, p. 20. Online version
Featured image: Promotional image for QL2's Belong, 2018. Photo: © Lorna Sim
Ariette Taylor Black Grace Dance diary David Hallberg Gideon Obarzanek Jacob's Pillow Liz Lea Meryl Tankard Nacho Duato Olivia Fyfe Quantum Leap/QL2 Remi Wortmeyer Sydney Dance Company
← Previous post Forever & Ever. Sydney Dance Company
Next postDon Quixote. La Scala Ballet →


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The Galveston Daily News. (Galveston, Tex.), Vol. 35, No. 133, Ed. 1 Saturday, June 12, 1875, newspaper, June 12, 1875; (https://texashistory.unt.edu/ark:/67531/metapth462138/m1/1/: accessed April 20, 2019), University of North Texas Libraries, The Portal to Texas History, texashistory.unt.edu; .


Three months and three days into 2019 and so far there's not too much on my schedule. But with spring ahead, some really decent tours are on the horizon and some will even head my way. While US-audiences always seem to get a much bigger piece of the cake, there's no reason to complain on my end.
Kicking off 13 days from today, Sweden's Lucifer will cross the big pond for an extended North-American tour with very special guests Spell. Furthermore the band will join forces with The Hellacopters to glance Europe with their collective Rock'n'Roll shenanigans.
And as the US will be welcoming yet another amazing tour package featuring King Dude and Maggot Heart, traveling the opposite direction, will be none other than Coven. After I missed out on their headlining appearance at Roadburn 2017 as well as the entire tour last year, I hope to finally catch of with Jinx Dawson and her fellow musicians as they return to European soil this summer.
Teaming up again this year will be Iceland's finest The Vintage Caravan and Belgium's very own Black Mirrors. After the first part of The Gateways tour last year, the two bands will hit the road once more throughout April and early May. Two years ago on this day, Black Mirrors released their eponymous debut EP. Their full-length followup "Look Into The Black Mirror" came out on August 30th, 2018. With their third album at hand, The Vintage Caravan will also be supporting Swedish Heavy Metal outlaws Bullet for a few selected dates.
Just a about a month ago my review on the past year was so much fun and I really look back on 2017 with a good feeling. And now that we're well into February, 2018 has already been quite a ride already. First off, my best friend finally made his way into the Metal-Olymp by joining veteran Thrash band SODOM. Looks like he's gonna be a real Rockstar after all. Besides, his own band BEYONDITION is much of a class act within the local underground itself. Offering a fine blend of Old School Death Metal in the vein of BOLT THROWER with a twist of Swedish Death to it. Guess I should try and do an interview with the guys to introduce them to the rest of the world. They are currently working on a debut album, with a 2017 demo sold out by now. Anyone who missed out on buying the tape: The demo is available as a full download via bandcamp. Totally looking forward to seeing them again soon!
Speaking of which, it only took me a good month to spend more money on concerts than I have in the past few years. And the amount that other people are willing to pay for the entire Wacken weekend, I will be celebrating two days of pure Rock'n'Roll awesomeness. After my failed attempt to see one of my all-time favorite bands at Rock Am Ring in 2006, this year will totally make up for it, as I will finally see GUNS N' ROSES with BOTH Axl and Slash sharing stages again! And to top it all, just one day later, QUEEN and ADAM LAMBERT are playing have a tour stop in Cologne. Only took me about eight years to catch up with Adam again. But I'm 100 percent sure that it will be totally worth the wait. Additionally, 2018 also marks my personal anniversary of ten consecutive years as an official press member at the annual Rock Hard Festival. Kicking off my run of live show shenanigans, will be the ever so amazing Linnéa Olsson with her very own MAGGOT HEART – featuring her former GRAVE PLEASURES bandmate Uno Bruniusson (PROCESSION, DEATH ALLEY, ex-IN SOLITUDE) on drums. With quite some more thins on my list of possible activities for the year ahead, including OZZY OSBOURNE, 2018 will really rock!
As the summer in the year of their lord 2017 draws near and the world in the north is again fully starting to wake from its slumber we, on the other hand, are forced to face an inevitable end in the departure of our drummer Jakob Ljungberg who has decided to leave the band. We have spent the last five years together through pain to heaven, in chaos to bliss! It's been such a strange, wonderful, tiring and inspiring time and we would like to thank you from the bottom of our hearts for making this time the most important in the history of the band. We surely couldn't have done it without you. We were like brothers even before the time of Tribulation and we certainly will be in the time after! Make sure to check out Jakob's unique and most excellent band Second Sun where he sings and plays guitar!
"It is with a heavy heart that I leave Tribulation. These last years have been among the best in my life, but they wore me out and now I have to continue life on different paths.
Thanks to everyone involved – you made this journey spectacular, thanks to everyone that came up and said hi – it meant the world to me, thanks to everyone who believed in me – you made me believe in myself. Jonathan, Adam and Johannes. I love you.
For Tribulation, however, this is not the end, but a new beginning. After this period of silence, renewal and contemplation the time has now come to give you the new Tribulation! We have now fully immersed ourselves in the making of a new album that will be recorded at summer's end.
We are very pleased to announce that Oscar Leander (previously in Deathstars) is our new drummer. He will make his first appearance with us on Muskelrock på Tyrolen now on Thursday, June 1st!
Though the band has been forced to cancel its appearance at Bang Your Head, they will play at Metal Magic Festival and Graspop Metal Meeting.
2016 started off with a rare moment as I had the first and unfortunately final chance the see Grave Pleasures in their best lineup, featuring Swedish guitarist Linnéa Olsson and former In Solitude drummer Uno Bruniusson. The now newly formed band was touring alongside Tribulation in January and gladly played a brilliant show at TuRock, Essen – not shying away from including several tunes from their former incarnation Beastmilk. Later this year I was lucky enough to see Tribulation again at Rock Hard Festival.
But before the outdoor season started, one of many indoor festivals caught my attention and had me attending – attempted pun intended – the second edition of Ván Records' very own Acherontic Arts Festival which took place in early May. Gathering the brightest shining gems of his artist roster, Sven clearly knows his way around a brilliant billing. Urfaust, Gold, the recently disbanded Path Of Samsara, The Ruins Of Beverast, to name but a few. My personal highlights have to be King Dude, who gave me all those emotions, from goosebumps, to shivers to tears and the outstanding performance of Germany's very own (D O L C H) – leaving me speechless and that rarely ever happens!
And then there was this: Rock Hard Festival – the only event I've been at almost every year since 2004. Second time watching Tribulation and for the first time in a while I could finally catch up with Kadavar again. Great to see these guys, that I've been a fan of and working with in a past life, making their way towards the big stages. This year also saw a premier, as I officially teamed up with Queen Of Spades Photography – run by my good friend and talented photographer Susan – to cover the mandatory reports.
In August it was finally time to look back the first five years of Psychorizon with a little festival. Four bands from three countries gathered at a local youth club to celebrate with me and my friends, fans, readers and the audience for one night. Even though only a handful of folks actually came around to enjoy the event, there shall be more live action to go about in the future. Special thanks to those who joined the party, my catering chef Cati and all members of the most brilliant opening act ArieZ, Swiss Stoner crew Drain and of course my amazing Canadian headliner Völur. Couldn't have done it without you, thanks so much! Spread the love and hope to see you all soon again!!!
And last but certainly not least, another most memorable night featured Ghost Bath and Thränenkind, who played at Helvete, Oberhausen on August 28th. While the main part of the audience was eagerly waiting to see the headliner, all I wanted was to finally see the band that created my personal favourite album of the year. Due to some scheduling difficulties, bass player Matthias and vocalist Nils had to borrow some stand-in musicians and still managed to deliver a stunning show. Hope they'll return to my area again soon!
Energetic Anarchy: Matthias the bass-machine!
This year has been a crazy ride and I'm really looking forward to all the adventures the next one will bring – hope we'll all make it a good one.
Fortunately, the reformed group, featuring British vocalist Mat McNerney, who now lives in Helsinki, remains as creative as ever. The A-Side contains the most catchy "Deadenders", which is already available in a powerful retro-style lyric video. Lyrical themes evolve around the end of the world of course, which will have us dance the Falloutpogo, as Mat advises us with his wonderfully striking voice.
The B-Side presents a slightly more moderate tune. This gem of a song is called "Cold War Funeral" and turns out to be a melancholy mushroom cloud, letting us swing once again.
Produced by John Davis, who has also worked with Lana Del Rey, the two tracks are the next step in the evolution of former Beastmilk. Specially the vocals have changed a lot compared to the 2015-album "Dreamcrash". Embetted a bit deeper into the mix, they have not lost their intensity and the light Danzig timbre.
In addition to a download via bandcamp, Mat's own label Secret Trees has a strictly limited 7 "version, each 300 black and 200 yellow.
After their most successful tour alongside countrymates Tribulation and Vampire in January, Grave Pleasures seem to have taken some time away from social media. As of today the band reveals one of the reason for their temporary withdrawal, seeing guitarist and former member of The Oath, Linnéa Olsson leaving them to pursue new adventures.
Commented the band: "We would like to thank Linnéa from the bottom of our hearts and wish her all the best on her new path. We will always be very proud of her and the work we did together. Grave Pleasures continues to rock and roll onward. We will announce our future plans very soon.
Grave Pleasures has been an intense adventure and creative experiment. This past year and a half has allowed me to grow as a songwriter and performer, and to experience life and music from strange and new perspectives.
Now the time is right for me to take the next step, and therefore I've made the decision to leave the band. I will focus on my own project, which hopefully will be in presentable shape later in the year!
A huge thank you to Uno, Juho, Mat & Valtteri, as well as all you people along the road for your much valued support. I hope to see you in the next chapter.
There's a new dark wave coming, black-flagged by bands like us and Tribulation (Official), who stretch their skeletal hands further out into the abyss of deathly rock. Each in our own directions, but sewn at the naval by shared influences, as children of the night-music. You're either with us or against us. Either way, we're happy to announce that we're going out on the road through Europe in January 2016 with Tribulation and Vampire in tow, to crash your dreams and drink your spirits. Fear the wailing of the dead!


text: TRUNCATE TABLE cr_heap_truncate_table;


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text:
Q: Proper type for OpenSQL IN operand I have function module which imports my_values
my_values is an custom internal table type of string.
This "my_values" variable contains for example: ["foo", "bar"]
I want to select all values from table Z_MYTAB where the column my_col is in my_values.
I tried this:
SELECT * FROM Z_MYTAB WHERE
       my_col in @my_values INTO TABLE @DATA(my_rows).

But this fails with an error message:

table my_values has wrong row structure

(The message was translated to English. The original could be slightly different)
I could loop over my_values but I would like to avoid this.
How to do SQL IN with host variables which are internal tables?

A: Selection with IN is possible only with a range table.
Conversion of an internal table into a range table can be done like this:
DATA ltr_value TYPE RANGE OF string.

ltr_value  = VALUE #( FOR <my_value> IN my_values
                      ( sign   = 'I'
                        option = 'EQ'
                        low    = <my_value> )
                    ).

A: IN openands could be of 2 types:
SELECT ... WHERE my_col IN ( value1, value2 , value3)

in this case no host expression can be used as right operand
SELECT ... WHERE my_col IN sel_tab[]

in this case sel_tab is a range like
So you could use the following:
DATA sel_tab type range of string.

sel_tab = value #( for ls in my_values ( sign = 'I' option = 'EQ' low = ls ) ).
SELECT * FROM Z_MYTAB WHERE
       my_col in @sel_tab[] INTO TABLE @DATA(my_rows).

Best regards

A: User JozsefSzikszai  pointed me to "SELECT FOR ALL ENTRIES".
I found this in the docs:

For an elementary row type, the pseudo component table_line must be specified for comp.

See: https://help.sap.com/doc/abapdocu_752_index_htm/7.52/en-US/abenwhere_logexp_itab.htm
IF my_values is initial.
  exit.
endif.

SELECT * FROM Z_MYTAB
  FOR ALL ENTRIES IN @my_values WHERE
  column_name = @my_values-table_line
  INTO TABLE @DATA(result_rows).

redpajama_set_name: RedPajamaStackExchange


text:
Alternative Mechanism approved GoI's 100% stake sale in CEL to Nandal Finance and Leasing Pvt. Ltd
AC Team
On November 29, 2021, over Rs 210 Crore bid by Nandal Finance and Leasing Pvt. Ltd received an approval from ministerial panel namely 'Alternative Mechanism' to acquire 100% equity shareholding of Government of India (GoI) in Central Electronics Ltd (CEL).
CEL is a CPSE (Central Public Sector Enterprises) under the Department of Scientific and Industrial Research (DSIR).
This is the second strategic stake sale by GoI after Air India.
Incorporated in 1996, Nandal Finance and Leasing Pvt Ltd is based in New Delhi, Delhi.
i.After this approval, the next step will be to issue the Letter of Intent (LoI) and then sign the Share Purchase Agreement. The whole process of disinvestment is expected to be completed during current FY22.
ii.This stake sale process has been carried out in a transparent manner which involved
Inter-Ministerial Group (IMG), Core Group of Secretaries on Disinvestment (CDG) and the empowered Alternative Mechanism (AM) at the apex Ministerial level.
They have been supported by Transaction Adviser (TA), Legal Adviser, Asset Valuer (AV) as professionals in their respective fields.
What is Alternative Mechanism?
Initiated in 2017 after Cabinet Committee on Economic Affairs (CCEA) approval, it is a framework to speed up and supervise the mergers of CPSEs, minority stake sales, and the Centre's new exchange traded fund.
It consists of the Finance Minister, Minister for Road Transport and Highways and minister representing respective administrative department
Currently, its composition is Union Ministers Nitin Jairam Gadkari, Ministry of Road Transport and Highways (MoRTH); Nirmala Sitharaman, Ministry of Finance; and Minister of State (Independent charge) Jitendra Singh, Ministry of Science and Technology.
The process for disinvestment of CEL commenced in October 2016. For this, two bidders submitted financial bids viz. Nandal Finance and Leasing Pvt Ltd for Rs 210 crore and JPM Industries Ltd bid for Rs 190 crore. The bid by Nandal Finance and Leasing Pvt Ltd was above the reserve price (fixed by TA & AV) of Rs 194 crore, therefore it has been selected for CEL sale.
Recent Related News:
In September 2021, Reliance Industries Limited's (RIL) subsidiary – Reliance Strategic Business Ventures Limited (RSBVL) acquired 57.06% stake in Strand Life Sciences by buying over 2.28 crore shares in the company for Rs 393 crores.
About Cabinet Committee on Economic Affairs (CCEA):
Chairperson– Prime Minister of India (Currently- Narendra Modi)
Composition– 9 (including Chairperson)
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text:
Q: SSIS package fails as a SQL Server Agent Job I have a package that imports from a AS400 file to SQL. The package executes properly within Visual Studio, but fails when set up as a scheduled job. the error message is that my password is incorrect. I know that it is correct. I also setup a package configuration and this did not work. I have searched and tried many things. Could someone give me some assistance?

A: Your password is incorrect.
Seriously, you "know" that your password is correct? You know better than the code attempting to use your password? Does this seem likely to you?
Consider the possibility that you and SSIS may be referring to different passwords. Maybe the one you "know" is correct actually is, but the other one is not.

A: Possibly a stupid answer, but how are you connecting to the AS400? If it's using ODBC drivers, you'll need the AS400 drivers installed on both local (dev) and your SQL server box.  They're notoriously picky about versions.
If memory serves me correctly, when you set up the ODBC connection using the AS400 driver software, I think you need to specify connection details as well and they get explicitly saved in the ODBC connection.

A: The support link above is correct. To boil it down to a simple answer. Password protect your SSIS package to save the credentials needed to connect to the AS400.

A: With the ODBC configuration: use a system DSN instead of user DSN, it will work!

A: Try to use odbc connection or try to redeploy the package on your SSIS Server.


text:
Centreville, AL (View All Cities)
Bibb County
Central (2:09pm)
Centreville, AL
Unacceptable:
Eoline
ZIP code 35042 is located in central Alabama and covers a slightly higher than average land area compared to other ZIP codes in the United States. It also has a slightly less than average population density.
The people living in ZIP code 35042 are primarily white. The number of people in their late 20s to early 40s is extremely large while the number of seniors is large. There are also a slightly higher than average number of single parents and a slightly less than average number of families. The percentage of children under 18 living in the 35042 ZIP code is slightly higher than average compared to other areas of the country.
Total 382 373 374 361 351 327 342 399 366 417 392 363 396 307 253 182 129 117
85 Plus 21 96 117
Renter 58 121 90 123 113 78 76 26
ZIP code 35042 has a slightly less than average percentage of vacancies. The Census also indicates that there are one or more nursing homes nearby.
The majority of household are owned or have a mortgage. Homes in ZIP code 35042 were primarily built in the 1970s or the 1990s. Looking at 35042 real estate data, the median home value of $94,500 is slightly less than average compared to the rest of the country. It is also slightly higher than average compared to nearby ZIP codes. So you are less likely to find inexpensive homes in 35042. Rentals in 35042 are most commonly 2 bedrooms. The rent for 2 bedrooms is normally $300-$499/month including utilities. 3+ bedrooms are also common and rent for $500-$749/month. Prices for rental property include ZIP code 35042 apartments, townhouses, and homes that are primary residences.
As with most parts of the country, vehicles are the most common form of transportation to places of employment. Compared to other ZIP codes in the country, 35042 has very few people that work at home. In most parts of the country, the majority of commuters get to work in under half an hour. A slightly higher than average number of commuters in 35042 can expect to fall in that range. Having to travel to work for over 45 minutes isn't uncommon for people who live here.
For more information, see Centreville, AL household income.
ZIP Code 35042 is in the following school districts: Bibb County School District and Private. There are 3 different elementary schools and high schools with mailing addresses in ZIP code 35042.
Brent Elementary School
1621 Montgomery Hwy.
Centreville, AL 35042
Grade Level: Middle/Elementary
District: Bibb County School District
Bibb County High School
220 Birmingham Rd
Cahawba Christian Academy
2415 Montevallo Rd
Brent, AL
Brierfield, AL
West Blocton, AL
Duncanville, AL
Maplesville, AL
Marion, AL
Randolph, AL
Lawley, AL


Get modern complete home interior with 20 years durability, richmond bedroom furniture set 2 door wardrobe, 4 2 chest, 3 pc pine bedroom furniture set wardrobe, 6 drawer chest. Homebase bedroom furniture wardrobes wwwindiepediaorg. Bedroom: beautiful wardrobe bedroom furniture 3 door.


text:
War of the Rebellion: Serial 012 Page 0515 Chapter XXIII. BATTLE OF WILLIAMSBURG, VA.
was moving up the branch road toward Hooker's position. General Casey and General Naglee had gone at the head of the column. I sent a staff officer immediately to find them, and in the mean time I dispatched the rear portion of the brigade myself [having faced it about] to the front from which I had come. The moment General Naglee joined me I returned in company with him, arriving at the White House about fifteen minutes before the arrival of the commanding general, and considerably in advance of the head of Naglee's column.
General McClellan sent for me and assumed command, and from him I received orders. The general quickly comprehended the state of the field and gave many directions to the fresh troops, ordering forward, among other troops, Naglee and his brigade, and the Tenth Massachusetts, Colonel Briggs, which advanced with great promptness to re-enforce Hancock, and in a very short time the battle ended in our victory.
As the forces engaged on the right in the battle of Williamsburg on the 5th instant belonged exclusively to the Fourth Army Corps, commanded by me, under Major-General McClellan, and as I was subject, until his arrival on the field, to the orders of Brigadier General E. V. Sumner, I have endeavored to confine my report principally to such facts as came under my own immediate observation and to such ideas as originated with me. The allusions made to Brigadier-General Sumner connected therewith are all, I think, sustained by the reports of commanders subordinate to me, and I desire that those reports may all be made public, and that a copy of my report be furnished to General Sumner.
The small number of troops actually in position early in the morning and our ignorance of the ground were most embarrassing circumstances. General Sumner received in my presence the most urgent appeals through General Stoneman and others to support Hooker by re-enforcements, and through General Smith and others, as well as through me, he was requested to support Hancock. His reasons for the orders he gave in answer to such solicitations it is not my province to know, nor do I pretend to say.
Confirming myself to the ideas suggested by the command of my own corps and to the time prior to the arrival of General McClellan on the field, I am bound to declare that I took the necessary precautions to have my three divisions in the presence of the enemy at an early hour of the day, but that, in spite of my efforts, there was but one there until the afternoon. If they had all arrived as early as 2 o'clock p.m., and if Hancock had been re-enforced as early as 3 o'clock p.m., the victory would have been one of the most brilliant of the war.
The commanders of the First, Second, and Third Divisions, Brigadier-Generals Couch, Smith, and Casey, have made reports, which, with the documents and reports attached to them, are herewith submitted. The names mentioned for praise in the various reports and the names of the killed, wounded, and missing will be forwarded as soon as the lists can be prepared. General Couch and General Smith [who was longest in the field] made excellent dispositions of their troops and were very active. Brigadier-General Casey arrived too late to take part in presence of the enemy, but he was prompt in dispatching a brigade to the support of Hancock and in maturing arrangements for the night. The enemy evacuated their works about 3 a.m. of the 6th, under cover of the darkness. Two companies of the Twenty-third Pennsylvania Volunteers, Colonel Neill, were the first to take possession of Fort Magruder, as that regiment had been the first to plant the Stars and Stripes on the works at Lee's Mill.
From the time of the movement to advance from Warwick Court-House
‹ Serial 012 Page 0514 THE PENINSULAR CAMPAIGN, VA. Chapter XXIII. up Serial 012 Page 0516 THE PENINSULAR CAMPAIGN, VA. Chapter XXIII. ›


The Pyrenees Mountain Range is physically beautiful, culturally varied and less developed than the Alps. Stretching 491km from the Bay of Biscay to the Mediterranean Sea, it forms a natural border between France and Spain. At the heart of the range is the Pyrenees National Park stretching 100km from east to west, from the Aure Valley to the Aspe Valley covering some 50,000 hectares.
With peaks rising to over 3,000 metres, an abundance of waterfalls and mountain torrents, 230 high-altitude lakes, vast areas of forest and masses of wildlife, the Pyrenees National Park is a stunning venue to have an adventure.
The expedition itinerary is a progressive phased programme of familiarisation/acclimatisation, qualifying expedition, rest and relaxation ensuring teams have the best chance of success on their qualifying expedition as well as ensuring they have an opportunity to get the most from their overseas expedition.
Teams arrive at Lourdes Airport and transfer to our base camp located in the Ski village of Cauterets in the heart of the Pyrenees National Park. They then get settled in before then venturing out into Cauterets to source the supplies they will need for the duration of their expedition. After a good nights sleep and an early start teams are taken out onto the local hills to get know the area and do specific in country training.
On day 3 teams wake up early and begin their 4 day Gold DofE qualifying expedition into the very heart of the Pyrenees. Going through and over the mountains they will follow sections of the world famous GR10 route and have stunning views of some of the route climbed by Tour de France cyclists including the legendary Col de Tourmalet, they will wild camp by high mountain lakes in the shadow of spectacular mountains such as the Pic du Midi. Each day as they journey they will have the opportunity to pursue their aim and discover the breath-taking views that the mountains have to offer. Each night they will camp in either a typical French valley-based campsite giving them an opportunity to practice their French with the locals or higher up in the mountains at a wild camp amongst towering mountains and emerald green lakes allowing them to fully absorb their surroundings.
On completion of their qualifying expedition and after a well-earned rest the teams will make a leisurely start to the day, they will have the opportunity to take in the local sights and attractions that the alpine village of Saint-Lary has to offer or if they are keen to do something a little bit more active then there are many other exciting options available. After a celebration meal in Saint-Lary we wake the following day to pack up and say goodbye to the Pyrenees. Teams then complete the short transfer from our campsite to the airport for their flight home.
Team equipment : high quality tents, stoves and cooking pans, fuel, group shelters, team first aid kits, maps, compasses, radios.


text:
Michigan Humane Society Opens $15.5 Million Animal Care Center In Detroit
Filed Under:Michigan Humane Society, Pet Adoption
DETROIT (WWJ) – The Michigan Humane Society is showing off its new multi-million-dollar facility in Detroit.
The MHS's state-of-the-art Detroit Animal Care Campus, on the I-75 Service Drive, opened its doors to the public for the first time on Monday, and WWJ's Vickie Thomas took the tour.
Spokesman Ryan McTeague showed off a well-lit room that houses adoptable cats.
"The first thing you'll notice is everything here is bright and airy," he told Thomas. "It's just great for reducing stress on cats because they really have a hard time adjusting to shelters…but you can see our kittens are enjoying their perches. We have big open areas."
New Detroit Animal Care Center (1)(credit: Vickie Thomas/WWJ)
New Detroit Animal Care Center (10)(credit: Vickie Thomas/WWJ)
"It's also, if you notice, very quiet," added McTeague. "You don't hear dogs barking."
The price tag for the place was $15.5 million which was all raised through donations made specifically for the facility.
"And we're very excited to be in this new building. We've been in Detroit for 139 years; been in our old building since 1931," McTeague said. "…We wanna make sure we thank everyone who helped us make this dream become a reality."
Lisa Ochoa, who was impressed by the new facility, came in with a dog she's fostering.
"Reagan came in with a fractured pelvis and something in his eye. It was an abrasion," she said. "We think he was run over by a car — completely run over —but he's doing really well now."
She said she plans to adopt the little guy.


(Born in 1990,Miyazaki Japan) is a Japanese jewelry design and creator.
Now live in Tokyo,and based in Atelier TOCOHA.
Jewelry production is often made mainly of acrylic and other resin materials and silver.
Her birth Miyazaki, Hyuga City had a mountain and a sea with a plaza that could see the land pattern and the cape. As her house was near the beach,she often bred in her family, went swimming, went out for a picnic, and touched nature.She loved to play outside and it was a sunburned girl like playing tags and balls with boys.As she grew up and belonged to the athletic club, her interest in art kept thin. However, since childhood she was taken to her mother and watched theater,went to her father and art museum, who liked art appreciation originally, and she was blessed with an opportunity to touch art.
Also, when she was a seventeen, her older brother went to art college and she started to get interested in art and design.Just when she went to see a sculpture exhibition she remembered vaguely that she wanted to make a job using her hands as a profession.Then she began to learn the drawing and entered Musashino Art University's Craft and Industrial Design Department.She majored in metal craftwork attracted by the nature of the metal and the work and personality of the professor.So, she encountered contemporary jewelry, she was shocked by not only metal but also the attractiveness and way of thinking of various materials.
Why is this form?Why use this material?Why is this wearing?
She was excited that a lot of '?' Emerged, and there is something that can drive her curiosity so much.It was the moment that common sense to her jewelry covered,and now it has just come to make jewelry.
Several years have passed since she finished graduate school and she works and presents works and sells mainly on galleries,department stores and web shops.
2013 Musashino Art University Department of Industrial, Interior and Craft Design,Metal work.


Noodlecake Studios with Woblyware and Ravenous Games have produced another simple 2D platformer that manages to be both interesting and consistently mundane. That isn't to say it isn't worth playing though.
The premise is that a massive Easter Island looking stone head wants you, a duck, to collect all his golden eggs. But this plot is barely given much thought- the chief draw here is the ability that the head bestows upon the duck- to flip gravity. You can't jump at all, you simply reverse gravity and fall in the opposite direction.
A giant stone head and a duck. What more could you ask for?
This simple new power is used in conjunction with some gravity rotating yellow orbs to solve roughly 100 levels of short puzzles. There is nothing to strenuous in terms of puzzles- nothing to rack your brain with- but the concept does prove to be fun enough to want to keep playing. The lack of challenge is low enough that you can nearly always tell what to do as soon as the level begins.
The downsides are the controls were occasionally unresponsive leaving players slightly frustrated when a lack of response movement leads directly to death. In addition, sometimes you need to dive blindly into areas and die because your view is severely limited in places (no camera movement). Once in a while the enemy laden areas need a bit of trial and error to figure out due to their swiftness, but it isn't too awful.
A fashionable top-hat is the reward for collecting all the golden eggs.
For only a dollar, Gravity Duck provides plenty of simple, cute, and pixely puzzling entertainment. Perhaps the gravity manipulation and level design for the coming "City" DLC will prove to add a little more variety for our entertainment. I hope they add some more progression, balance, and flow to the levels and challenge to come- I would like more of a sense of achievement from the puzzles- something a little more like a 2D version of the phenomenal PS Vita game Gravity Rush. There is a wide range with the concept they've used, if only they'd take it to the next level of its potential.


life") is the traditional Japanese art of flower arrangement, also known as Ikebana.
of the Rising Sun, to seasons well marked by cultural and ancestral patterns."
KADŌ meaning «the way of flowers» or «the art of bringing flowers to life» is the traditional Japanese art of flower arrangement, also known as Ikebana. Through the freshness of the seasonal rainwater, a wave of aromatic tea and floral sweetness enchants and leads us on a journey through the traditions of the Land of the Rising Sun, to seasons well marked by cultural and ancestral patterns.
The essential oil of yuzu has numerous relaxing virtues because it helps to fight against the stress, the fatigue and warns the difficulties to fall asleep. Its formula base on alcohol of Organic Wheat is guaranteed without phtalates, without parabens !
INGRÉDIENTS /состав : Alcohol Denat, Aqua(Water), Parfum(Fragrance), Limonene, Linalool, Geraniol, Benzyl Alcohol, Benzyl Benzoate, Benzyl Sallicylate, Citronnellol, Citral, Farnesol, Isoeugenol.
* Our wood comes from France, Spain and Belgium and is certified PEFC who guarantee the sustainable management of forest.


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Conferences and Events at NPS
How Much and on What?
Powell_HOW_MUCH_AND_ON_WHAT_CIP_Metrics_Tools_2008.pdf (140.2Kb)
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Powell, Robert
How much should a defender spend on defense and how should it allocate those resources across the sites it is trying to protect? This paper analyzes a model in which a defender first has to decide how much to spend on defense and what to spend it on. The more that a defender devotes to protecting a specific site, the less likely an attack on that site is to succeed and, crucially, the lower the marginal return to investing in attacking that site. After the defender moves, the attacker decides how much effort to devote to attacking each site. Three key conclusions result: First, the questions of how much to spend and what to spend it on are "separable." However much the defender decides to spend, it should allocate those resources in the same general way. Second, a very simple principle or algorithm determines the optimal allocation. The defender minmaxes the attacker's marginal gains, i.e., allocates its resources in the way that minimizes the attacker's maximum marginal gain from exerting additional effort. Third, the defender is in effect a Stackelberg leader. The optimal level of spending takes into account how the defender's allocation affects the attacker's effort and generally is that level of spending which equates the marginal benefits of additional spending with the marginal cost of diverting these resources from other social ends.
How Much and on What?
Powell, Robert (2008-06);
How much should a defender spend on defense and how should it allocate those resources across the sites it is trying to protect? This paper analyzes a model in which a defender first has to decide how much to spend on ...
The Fast Theater Model (FATHM) Optimization of air-to-ground engagements as a defender-attacker model
Seichter, Stephan (Monterey California. Naval Postgraduate School, 2005-12);
The FAst THeater Model (FATHM) is a joint theater-level attrition model that combines a Lanchester ground combat model with a linear program, hereafter the Air model, that determines the optimal allocation of air strikes ...
Network Optimization Models for Resource Allocations in Developing Military Countermeasures
Golany, Boaz; Kress, Moshe; Penn, Michael; Rothblum, Uriel G. (2012);
A military arms race is characterized by an iterative development of measures and countermeasures. An attacker attempts to introduce new weapons in order to gain some advantage. whereas a defender attempts to develop ...