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Home » Faculty & Staff, Mobile
NECC Professor's Work Highlighted in New MIT Press Book
Submitted by on February 13, 2015 – 6:56 pm
NECC professor and Merrimac resident Lance Hidy has contributed a chapter to "The Eternal Letter," a new book published by MIT Press. The book, which was released this winter in conjunction with the two thousandth anniversary of the classical Roman capital letter, explores the evolution and significance of Roman typography through essays by renowned carvers, typographers, linguists, graphic designers, and other experts in letterforms. It is now available for sale.
As a design expert, Hidy provides a comprehensive look at the process involved with developing and implementing a font family. His ten-page chapter "Penumbra: the Offspring of Trajan and Futura," discusses his work in creating a new font type inspired by classic Roman letterforms and modernized through poster art. The Penumbra font family was published by Adobe Systems in 1994. In 2006 Penumbra was selected as the promotional poster font for "The Da Vinci Code," a blockbuster starring Tom Hanks.
Lance Hidy is a native of Portland, Oregon who got his start in design and illustration after graduating from Yale University and studying privately with the sculptor and printmaker Leonard Baskin. In 1969, he co-founded the company David R. Godine, Publisher and four years later established a design firm of his own. By the 1980s, Hidy had gained a strong reputation for his expertise in poster art and illustration, eventually serving as the art director of the Harvard Business Review and designing three U.S. postage stamps. Hidy currently teaches graphic design and history part-time on Northern Essex Community College's Haverhill campus.
NECC's art and design program prepares students for work in multi-media or fine arts fields and for transfer to four-year programs. For more information on the program, please visit www.necc.mass.edu/academics/courses-programs/areas/design.


With the Dassel-Cokato Performing Arts Center (PAC), the DC community is able to bring in big-city entertainment year-round, such as the Minnesota Orchestra and the a capella group, Tonic Sol-fa.
The PAC was built in 2004, and began entertaining audiences with big name acts in 2005. The 800-seat, air-conditioned auditorium is located on the DC high school and middle school campus. The state-of-the art sound and light equipment gives a professional theatre atmosphere.
Copyright City of Cokato. All Rights Reserved.


NFL teams won't stop looking for ways to improve just because the 2016 NFL draft is over. Plenty of general managers are working the phones Saturday night to sign players who went undrafted.
This time last year, the Seattle Seahawks were in the process of adding running back Thomas Rawls. The 22-year-old appeared in 13 games, rushing for 830 yards and four touchdowns. With Marshawn Lynch retired, Rawls is in line to be the starting running back in Seattle in the upcoming season.
Cincinnati Bengals linebacker Vontaze Burfict is another success story, making the Pro Bowl two years after he slipped out of the 2012 draft.


oscar777 This post is not being displayed .
Any of you boys(and girls) going down to Peterborough this weekend?
The last post was made 2 years, 339 days ago. Instead of replying here, would creating a new thread be more useful?


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Казан-чункур () — упразднённое село в Жарминском районе Восточно-Казахстанской области Казахстана. Входило в состав Бирликшильского сельского округа. Код КАТО — 634447300. Ликвидировано в 2013 году.

Население
В 1999 году население села составляло 115 человек (63 мужчины и 52 женщины). По данным переписи 2009 года, в селе проживало 40 человек (25 мужчин и 15 женщин).

История
В 1942—1953 годах Казаншункур имел статус рабочего посёлка.

Примечания

Упразднённые населённые пункты Жарминского района

redpajama_set_name: RedPajamaWikipedia


A solid oak chair with a deeply brushed surface to expose the grain, finished in a black lacquer. The Slab Chair was born out of the need for a stackable, space-saving armchair. The Slab Chair is also available in a natural lacquer.The Slab collection includes a dining table, bench and a bar stool.


Golden Bonbon Nougat New Arrival Stocks!
Another GOOD NEWS!!! Latest SAMYANG LIMITED EDITION Cool & spicy noodles from Korea is HERE!! Now available at Ta Kiong Kuching, Miri & Sibu.
GOOD NEWS! The Famous Samyang Noodles are BACK AGAIN!!! Grab them now at Ta Kiong at Super Value Price.


text:
Cuban leader invited to visit Russia
President Miguel Diaz-Canel took office in April 2018
© EPA-EFE/MICHAEL REYNOLDS
UN, September 25. /TASS/. Cuban President Miguel Diaz-Canel is invited to visit Russia, Russian Foreign Minister Sergey Lavrov told journalists in reply to the question about a possible meeting between Russian and Cuban leaders.
"He [Diaz-Canel] has an invitation to visit Russia," Lavrov said on the outcomes of the talks with his Cuban colleague Bruno Rodriguez on the margins of the UN General Assembly's session.
"Today, we have considered upcoming contacts planned at a political level, including in the context of discussing the current issues of our economic cooperation," Lavrov added, commenting on the outcomes of the meeting. "We are preparing a session of the intergovernmental commission. Of course, we have discussed the coordination of actions at the UN."
Miguel Diaz-Canel replaced Raul Castro as President of Cuba's Council of State and President of the Republic of Cuba in April 2018.

redpajama_set_name: RedPajamaCommonCrawl


text:
Why do wheels sometimes seem to move slowly in old films?
Rollin' rollin' rollin'... wagon wheels in old movies sometimes appear to move in slow motion.
By Robert Matthews
Asked by: Robin Chambers, Preston
Films are shot as a series of individual frames taken at around 24 per second. If the wagon wheel is rotating at precisely the right rate, then a spoke in one frame will have been taken up by another spoke in the next frame, creating the impression the wheel is stationary. If they're slightly out of sync, however, the wheels will appear to move in slow motion.
Robert Matthews
Robert is a science writer and visiting professor of science at Aston University. He likes maths, West End musicals and hamsters.


PALMETTO, FL (WWSB) – The Ringling Brothers Barnum and Bailey train car has been moved from Palmetto to the Showpeople's Winter Quarters in Seffner.
The site is home to a retirement facility for those who worked in the circus industry. The train car was built in 1953 for the Union Pacific Railroad. In 1972, Feld Entertainment acquired it and converted it.The unit stayed in operation with the circus until the very last show earlier this year.The train car will be converted in a community center at it's new home on Highway 932 in Hillsborough County.
A shame to see it go.


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Right Wing Brief
Home Politics Trump pardons Paul Manafort, Roger Stone and Charles Kushner
Trump pardons Paul Manafort, Roger Stone and Charles Kushner
President Trump announced 26 new pardons Wednesday, including for allies Paul Manafort and Roger Stone, as well as Jared Kushner's father, Charles Kushner. Mr. Trump granted 15 pardons the day before.
Manafort, a former Trump campaign manager, was sentenced to 7-and-a-half years in federal prison for convictions related to former special counsel Robert Mueller's Russia investigation. Manafort was released from prison in March to serve his sentence from home due to COVID-19.
Mr. Trump had already commuted the sentence of Stone, a longtime friend, in July. Stone was convicted of seven felony counts stemming from Mueller's investigation, including lying to investigators and witness tampering.
Kushner was convicted of witness tampering, tax evasion and illegal campaign contributions back in 2005. Jared Kushner, Mr. Trump's son-in-law, has worked in the White House since the beginning of Mr. Trump's presidency, and has been one of the president's most influential and long-serving aides. The case against Charles Kushner was prosecuted by former New Jersey Governor and Trump ally Chris Christie.
The pardon announcement comes as the president arrives in Florida for his Christmas vacation, after vetoing the National Defense Authorization Act and threatening not to sign the stimulus package that would grant relief for millions of Americans. Mr. Trump pardoned other allies and former Republican members of Congress earlier this week.
Manafort immediately took to Twitter to thank the president.
"Mr. President, my family & I humbly thank you for the Presidential Pardon you bestowed on me. Words cannot fully convey how grateful we are," he tweeted.
Although presidential pardon powers are broad, they are generally intended to be granted to those who have atoned for their transgressions, expressed remorse for their actions, and often served society in some way. That is not the case with most of the recent pardons of the president's allies.
Andrew Weissmann, a senior prosecutor in Robert Mueller's special counsel investigation, blasted the president for the move on Twitter.
"The pardons from this President are what you would expect to get if you gave the pardon power to a mob boss," he wrote.
The president even received harsh criticism from some Republicans.
"This is rotten to the core," said Nebraska Senator Ben Sasse in a six-word statement.
But Mr. Trump cannot protect his allies from state prosecution, which could be around the corner.
"This action underscores the urgent need to hold Mr. Manafort accountable for his crimes against the People of New York as alleged in our indictment, and we will continue to pursue our appellate remedies," said Danny Frost, director of communications for Manhattan District Attorney Cyrus Vance Jr.
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They are certainly finding it and a lot more.
The Cardinals also gaining momentum and some obvious confidence, something the perennial playoff contenders looked to be missing while losing seven of their first 12 games.
The Cardinals will send ace Carlos Martinez to the mound Sunday at Great American Ball Park to try to finish sweeping a four-game series against the struggling Reds.
St. Louis has outscored the Reds 24-8 in the series. They won 6-1 Saturday behind utility man Greg Garcia's two home runs, Tommy Pham's three hits and starter Miles Mikolas' seven effective innings of one-run pitching.
Cardinals manager Mike Matheny marveled how effective Garcia is coming off the bench. Garcia, who rarely plays against left-handers, had never had a multiple-homer game or homered off a left-hander until he went deep twice against Reds left-hander Brandon Finnegan, raising his average to .333.
"It's hard to explain how hard that is to do," Matheny said of Garcia managing to stay sharp despite limited playing time and at-bats. "Wow. Great at-bats. He's impressive, how he stays sharp and how he's ready to go."
Garcia's big day was the latest addition to a Cardinals offense that has produced 33 hits -- 15 for extra bases -- against the Reds this weekend.
Their three wins in Cincinnati have pushed the Cardinals over .500 for the first time this season. The Cardinals also dropped the Reds to 2-12 with seven consecutive losses in which they've been outscored 45-17.
It wasn't supposed to be nearly this bad for the Reds, even though they're coming off three consecutive last-place seasons in which they averaged 95 losses. Now, they're off to their worst start in 87 years, or since they also were 2-12 in 1931, when they lost 96 times during a 154-game season.
Reds manager Bryan Price wasn't about to lay blame on Finnegan, who was making his first start of the season, but it's obvious he expected more from the left-hander.
Finnegan (0-1) labored through 4 1/3 innings, allowing five runs and six hits, walking four and giving up three two stolen bases -- two to Pham, who is hitting .327.
"He wasn't real sharp. He had a hard time getting things going," Price said. "He was pretty deliberate to the plate and they were able to take advantage of that. I anticipate him getting better, but I was expecting him to be more sharp."
Price will send his top starter, Homer Bailey (0-2, 3.24 ERA) to the mound Sunday to try to salvage the final game of the series, but the right-hander doesn't have a good track record against the Cardinals, a team he hasn't beaten since May 23, 2014.
Bailey was 0-2 with 14 earned runs allowed in 7 1/3 innings against St. Louis last season and is 0-3 against them since 2015. He is 6-13 with a 5.86 ERA against the Cardinals overall in 23 career starts.
Bailey allowed one run on two hits in six innings and took a no-decision in a 6-1 loss at Philadelphia on Tuesday. He pitched 5 1/3 hitless innings and struck out seven.
"Homer did a spectacular job," Price said. "That's a big step for him."
Matt Carpenter (18-for-33), Yadier Molina (15-for-39, three home runs, 6 RBIs) and Kolten Wong (6-for-12) have done considerable damage against Bailey.
Martinez has had more success against the Reds, going 6-3 with a 3.84 ERA in 19 appearances (eight starts), although he was only 1-2 against them last season. Martinez (1-1, 2.41 ERA, 9.16 strikeouts per nine innings) is coming off a 5-3 victory Tuesday over the Milwaukee Brewers in which he allowed one run over six innings.
"Did you see my new pitch?" Martinez said to reporters after that outing.
Martinez already threw four-seam and two-seam fastballs but now, at the suggestion of Cardinals right-hander Adam Wainwright, is also throwing a cut fastball that's proving to be effective against left-handed hitters. He threw it an estimated 21 times against the Brewers.


text:
\section{Introduction}
Axions are copiously produced at the QCD phase transition. A possible way to detect these cosmological axions is through the observation of lasing axion clouds (clumps). If axions are a component of the cold dark matter (CDM), they can form density perturbations in the early Universe. If the over dense regions have high enough number density, then ambient photons from the cosmic microwave background (CMB) or from spontaneous axion decays, can induce stimulated  axion decay within the clumps, i.e., the axions can lase \cite{Kephart:1986vc,Tkachev:1987cd,Kephart:1994uy}.

Besides the initial clumps, other axion structures can form. The initial density perturbations can infall and evolve to form caustics \cite{Sikivie:1997ng} which have complicated geometries. Yet another possibility is that axions can be produced after the formation of primordial black holes (PBHs). Such black holes can be the results of various early universe processes, from cosmic string or domain wall singularities to density perturbations. However they for, if they have sufficient angular, either initially or from mergers, then superradience can occur causing axions to populate an $n,l,m=2,1,1$ hydrogen-like orbit around them if the axion Compton wavelength is comperiable to the PBHs' radius. If the axion density is high enough they can lase \cite{Rosa:2017ury}. The process can saturate, stop and then repeat in what is similar to what has been seen for fast radio bursts (FRBs).

Lasing in the PBH superradience case has so far only been approximated using the sphyerically symmetric model \cite{Rosa:2017ury}. In this work and in \cite{Chen:2020ufn} we point the way to an improving this approximation using multipole expansions of the spatial and momentum space distributions to more closely represent the physical axion distributions expected around a PBH.

\section{Photon angular distribution}
In \cite{Kephart:1986vc,Kephart:1994uy} nonrelativistic axions of mass $m_a$ were contained in a ball of radius $R$, with a maximum momentum value of $p_{\textrm{\tiny max}} \approx m_a\beta$. Here we allow a non spherically symmetric spatial distribution $X(\theta,\phi)$ to modify the axion clouds model previously studied, with the aim of finding the angular distribution $Y(\theta,\phi)$ of photons resulted from decays of axions, providing that there is some outside constraint (e.g., a gravitational field or self interactions) that can keep the axions  in the initial spatial distribution. For such an axion distribution, assuming it factorizes, the occupation number $f_a(p, r, \theta, t)$ and number densities $n_a(r, \theta, t)$ can be written
\begin{flalign}\label{axionON}
& f_a(p, r, \theta, t) =f_{ac}(t)\Theta(p_{\textrm{\tiny max}}-p)\, \Theta(R-r)  X(\theta)  \\ \nonumber
\end{flalign}
and
\begin{flalign}
&  n_a(r, \theta, t) =\int\frac{d^3p}{(2\pi)^3} f_a(p, r, \theta, t)  \\ \nonumber
&\qquad\qquad = \frac{m_a^3\beta^3}{6\pi^2} f_{ac}(t) \Theta(R-r) X(\theta)  \\ \nonumber
&\qquad\qquad =n_{ac}(t)\Theta(R-r) X(\theta)   \label{axion-fn}
\end{flalign}
where we can translate between the two with
\begin{flalign}
 f_{ac}(t) =\frac{6\pi^2}{ m_a^3 \beta^3} n_{ac}(t) .
\end{flalign}

Here and elsewhere we use the short hand notation $X(\theta)$ for $X(\theta,\phi)$, likewise for $Y$, $f$ and $n$.

The photons are contained in a ball of radius $R$, a momentum spherical shell of inner and outer radius $k_-  =\frac{m_a\gamma}{2}(1-\beta)$ and $k_+ = \frac{m_a\gamma}{2}(1+\beta) $ respectively \cite{Kephart:1994uy}, where we use $\beta =v/c$.
\begin{flalign}\label{photonON}
& f_\lambda(k, r, \theta, t) = f_{\lambda c}(t) \Theta(k_+-k) \Theta(k-k_-) \Theta(R-r)Y(\theta)    \\ \nonumber
\end{flalign}
and
\begin{flalign}
 &n_\lambda( r, \theta, t)   = \int\frac{d^3k}{(2\pi)^3} f_\lambda(k, r, \theta, t)  \\ \nonumber
&\qquad\qquad = f_{\lambda c}(t)\Theta(R-r)Y(\theta) ~ {V_k \over 8\pi^3 }   \\ \label{5}
&\qquad\qquad = n_{\lambda c}(t)\Theta(R-r)Y(\theta)   \nonumber
\end{flalign}
with
\begin{equation}
   f_{\lambda c}(t) = \frac{8\pi^2 }{ m_a^3\beta }  n_{\lambda c}(t)  \label{photon-rel}
\end{equation}
where $f_\lambda(k, r, \theta, t)$ and $n_\lambda( r, \theta, t)$ are the photon occupation number and photon number density,  of helicity $\lambda=\pm1$ respectively, which are related by eq.(\ref{photon-rel}) and $V_k$ is the volume of the momentum spherical shell
\begin{flalign}\nonumber
V_k &= \int_{k_-}^{k_+} d^3k = 4\pi ({m_a\gamma \over2})^2 (k_+-k_-)= \pi m_a^3\beta\gamma^3 \approx \pi m_a^3\beta .
\end{flalign}

We assume that the number density of each helicity state is the same, so the total photon number density $n_\gamma$ can be written as
\begin{flalign}\nonumber
 n_\gamma( r, \theta, t) &= n_{\gamma c}(t)\Theta(R-r)Y(\theta)  = n_+( r, \theta, t) + n_-( r, \theta, t) &&\\ \nonumber
&= [n_{+c}(t)+n_{-c}(t)]\Theta(R-r)Y(\theta)  &&\\
 n_{+c}(t) &= n_{-c}(t) \qquad n_{\gamma c}(t)=2n_{\lambda c}(t)  \label{lambda-gamma}
\end{flalign}
which defines $n_{xc}$.
Hence the coefficient of the total photon number density is just 2 times that of photon number density of each helicity state.

  The evolution relation between axion and photon occupation numbers is (see equation (13) of \cite{Kephart:1994uy})
\begin{flalign} \label{13Kephart}
&\frac{d f_\lambda ( k )  }{dt} =\frac{m_a \Gamma_a}{k^2} \int_{\frac{m_a^2}{4k}} d k_1     \\ \nonumber
&\times \{  f_a  ( k+k_1 ) [ 1+ f_\lambda ( k ) + f_\lambda ( k_1 ) ] - f_\lambda ( k )f_\lambda ( k_1 ) \}
\end{flalign}
where $f_\lambda ( k )$ and $f_\lambda ( k_1 )$ are photon  occupation numbers of momentum $k$ and $k_1$, respectively. Other variables in $f_\lambda ( k )$ and $f_\lambda ( k_1 )$, i.e. $r, \theta, t$, are the same since they share the same spacetime. $ f_a  ( k+k_1 ) $ is the axion occupation number of momentum $k+k_1$. $\Gamma_a$ is the spontaneous axion decay rate.

This evolution equation can be integrated over $k$ and $k1$ phase space to yield (see the Appendix)

 %
\begin{flalign} \nonumber
\frac{d n_\lambda  }{dt}
&= \Theta(R-r)  \frac{m_a^3 \Gamma_a}{ 8\pi^2 } \bigg\{    [f_{ac} ( x + 2f_{\lambda c} \, xy    ) -f_{\lambda c}^2  y^2 ]   \times &&\\ \label{9}
&\quad [2\gamma^2\beta -\ln\bigg( \frac{1+\beta}{1-\beta} \bigg) ] - f_{\lambda c}^2  y^2 \times (2 \gamma^2\beta^2    ) \bigg\}
\end{flalign}

Now we employ the nonrelativistic approximation ($\beta\ll1$).
\begin{flalign} \nonumber
& 2\gamma^2\beta = \frac{2\beta}{1-\beta^2} \approx 2\beta(1+\beta^2) = 2\beta + 2\beta^3    \\ \nonumber
& \ln\bigg( \frac{1+\beta}{1-\beta} \bigg) \approx 2\beta + \frac{2\beta^3}{3}      \\ \nonumber
& 2 \gamma^2\beta^2 \approx  2\beta^2
\end{flalign}
to arrive at
\begin{flalign} \nonumber
&\frac{d n_\lambda  }{dt} =   \Theta(R-r)   \\ \nonumber
&  \times \frac{m_a^3 \Gamma_a  \beta^2  }{ 6\pi^2 } \bigg\{    f_{ac} ( X + 2f_{\lambda c} \, XY    )\beta - ( \beta + { 3\over2} )     f_{\lambda c}^2  Y^2     \bigg\}
\end{flalign}

Substituting  the derived relations \eqref{axion-fn} and  \eqref{5}  into  \eqref{9}
\begin{flalign} \nonumber
\frac{d n_\lambda  }{dt} &= \Gamma_a \Theta(R-r)  &&\\ \nonumber
&\qquad  \times\bigg[  n_{ac} ( X + \frac{ 16 \pi^2 n_{\lambda c} }{ \beta m_a^3 }  XY   )
- \frac{ 32 \pi^2 n_{\lambda c}^2 }{ 3 m_a^3 } (\beta + \frac{3}{2} ) Y^2  \bigg]  ~.
\end{flalign}
Taking into consideration photon surface loss
\begin{flalign} \nonumber
\bigg( \frac{d n_\lambda  }{dt}  \bigg)_{\textrm{  surface loss}}  = - \frac{3c n_\lambda}{2R}
= - \frac{3c}{2R} n_{\lambda c} \Theta(R-r) Y(\theta)   ~,
\end{flalign}
we have an equation which gives the  number density for each helicity state
\begin{flalign} \nonumber
\frac{d n_\lambda  }{dt}  &=   \Theta(R-r) \times \bigg[  \frac{n_{ac}}{\tau_a} X(\theta) +
\frac{ 16 \pi^2 n_{ac} n_{\lambda c} }{ \beta m_a^3 \tau_a }    X(\theta)  Y(\theta)     &&\\  \nonumber
&\quad   - \frac{ 32 \pi^2 n_{\lambda c}^2 }{ 3 m_a^3 \tau_a } (\beta + \frac{3}{2} ) Y(\theta)^2
- \frac{3c  n_{\lambda c} }{2R}  Y(\theta)   \bigg]     &&\\ \nonumber
\end{flalign}
where we are assuming, as was shown in \eqref{lambda-gamma}, that total number density of photon is twice that of the individual helicity states. Therefore the rate of change of total number density of photon is
\begin{flalign} \nonumber
\frac{d n_\gamma  }{dt}  &=   \Theta(R-r) \times \bigg[  2 \frac{n_{ac}}{\tau_a} X(\theta) +
\frac{ 16 \pi^2 n_{ac} n_{\gamma c} }{ \beta m_a^3 \tau_a }   X(\theta) Y(\theta)    &&\\  \nonumber
&\quad - \frac{ 16 \pi^2 n_{\gamma c}^2 }{ 3 m_a^3 \tau_a } (\beta + \frac{3}{2} ) Y^2(\theta)
- \frac{3c  n_{\gamma c} }{2R}  Y(\theta)   \bigg]     ~.
\end{flalign}

  Since from  \eqref{lambda-gamma}
\begin{flalign}\nonumber
\frac{d n_\gamma  }{dt} & = \frac{d n_{\gamma c}  }{dt} \Theta(R-r) Y(\theta) ~,
\end{flalign}
if we drop the step function $\Theta(R-r)$
we have an equation for the coefficient of total number density of photon
\begin{flalign}\label{photoncoeff1}
\frac{d n_{\gamma c}  }{dt}  &= 2 \frac{n_{ac}}{\tau_a} \frac{X(\theta)}{Y(\theta)} +
\frac{ 16 \pi^2 n_{ac} n_{\gamma c} }{ \beta m_a^3 \tau_a }    X(\theta)    &&\\  \nonumber
&\quad  - \frac{ 16 \pi^2 n_{\gamma c}^2 }{ 3 m_a^3 \tau_a } (\beta + \frac{3}{2} ) Y(\theta)
- \frac{3c  n_{\gamma c} }{2R}   ~.
\end{flalign}
From the first to the last term on the right hand side(RHS) of the equation, the terms account for spontaneous decay of axions, photon stimulated decay of axions, back reaction of photons, and surface loss of photons, respectively. Following similar approach, we  obtain an equation regarding the coefficient of total number density of axions
\begin{flalign}\label{axioncoeff1}
\frac{d n_{a c}  }{dt}  &= - \frac{n_{ac}}{\tau_a} \frac{X(\theta)}{Y(\theta)} -
\frac{ 8 \pi^2 n_{ac} n_{\gamma c} }{ \beta m_a^3 \tau_a }    X(\theta)
+ \frac{ 8 \pi^2 n_{\gamma c}^2 \beta }{ 3 m_a^3 \tau_a } Y(\theta)    ~.
\end{flalign}

The third term on the RHS of \eqref{axioncoeff1} is proportional to $\beta$, while the third term on the RHS of \eqref{photoncoeff1} has a factor of $(\beta+{3\over2} )$.  Keeping track of two parts of axions generated from the back reacting  photons, we find that the ${3\over2}$ in the third term on the RHS of \eqref{photoncoeff1} represents sterile axions and it should have been and was excluded in the derivation of \eqref{axioncoeff1}.\\
\indent The left hand sides (LHS) of  \eqref{photoncoeff1} and \eqref{axioncoeff1} have no $\theta$ dependence, but the RHS does. $X(\theta)=Y(\theta)$ won't make \eqref{photoncoeff1} and \eqref{axioncoeff1} valid simultaneously. So even if there is some outside constraint which can keep the axions in the $X(\theta)$ distribution fixed, the photons cannot have the same distribution, i.e., $Y(\theta)\neq X(\theta)$.\\
\indent There is no simple way to find a closed form for $Y(\theta)$ because the LHS of the equations \eqref{photoncoeff1} and \eqref{axioncoeff1} have no $\theta$ dependence, while the $\theta$ dependences on the RHS of these equations are different. This suggests the possibility that  $Y(\theta)$ may be found as a series expansion in $X(\theta)$. As a first test of this idea we replaced the general form $X(\theta)$ with $\sin\theta$ to study the distribution with more axions accumulated near the equatorial plane with few near the polar area, aiming at matching orders of $\sin\theta$ on each side of equations. But this fails as it turns out that $\sin^n \theta ~ (n\in\mathbb{Z})$ is not an orthogonal set of functions and thus the calculation leads to contradictions. Therefore, we must expand the occupation numbers and number density in terms of a full set of orthogonal  functions. We do this in the next section where we choose the set to be the real spherical harmonics.

\section{Real sperical harmonics expansion}
The  set-up here is similar to the previous discussion except that the axion and photon occupation numbers and number densities have coefficients labeled by order index $l$ and $m$. For the axions
\begin{flalign}\nonumber
f_a(p, r, \Omega, t) =& \sum_{lm}f_{a lm}(t)Y_{lm}(\Omega)  \Theta(p_{\mbox{\tiny max}}-p)\, \Theta(R-r)    \\ \nonumber
  n_a(r, \Omega, t)=& \sum_{lm} n_{a lm}(t) Y_{lm}(\Omega)   \, \Theta(R-r)  \\ \nonumber
  f_{a lm}(t) =& \frac{6\pi^2  }{ m_a^3 \beta^3}  n_{a lm}(t)   \end{flalign}
where we have set
\begin{flalign}\nonumber
f_{ac}(t)X(\theta)= \sum_{lm} f_{a lm}(t) Y_{lm}(\Omega)
 \end{flalign}
Note that  $n_a$ can not be any superposition of real spherical harmonics, it  has to be real and positive, so it should be   put into the form
\begin{flalign} \nonumber
 n_a =& \Theta(R-r)   ( \sum_{l'm'} n_{a l' }^{m'}   Y_{l'}^{m'} )^*  (\sum_{lm} n_{a l }^m   Y_l^m  )  ~,
\end{flalign}
where $Y_l^m$ are complex spherical harmonics. This also applies to photons.
\begin{flalign}\nonumber
 f_\lambda(k, r, \Omega, t) =& \sum_{lm}f_{\lambda lm}(t)Y_{lm}(\Omega)       \\ \nonumber
&\times  \Theta(R-r) \Theta(k_+-k) \Theta(k-k_-)   \\ \nonumber
 n_\lambda( r, \Omega, t)  =& \sum_{lm}n_{\lambda lm}(t)Y_{lm}(\Omega)  \Theta(R-r)      \\ \nonumber
 f_{\lambda lm}(t)  =& \frac{8\pi^2  }{ m_a^3\beta } n_{\lambda lm}(t)
\end{flalign}
\begin{flalign}\nonumber
 n_\gamma( r, \Omega, t)
=&  \sum_{lm}[n_{+ lm}(t)+ n_{- lm}(t)]Y_{lm}(\Omega)  \Theta(R-r)     \\ \nonumber
=&    \sum_{lm}n_{\gamma lm}(t)Y_{lm}(\Omega)  \Theta(R-r)      \\ \nonumber
n_{+ lm}(t)  =&   n_{- lm}(t)      \qquad
n_{\gamma lm}(t)  = 2n_{\lambda lm}(t)
\end{flalign}
where similar the the axion case we have set
\begin{flalign}\nonumber
f_{\lambda c}(t)Y(\theta)= \sum_{lm} f_{\lambda lm}(t) Y_{lm}(\Omega).
 \end{flalign}
Following the steps from the previous general discussion, we have an equation similar to \eqref{photoncoeff1} for each choice of $lm$
\begin{flalign} \label{photoncoeff2}
 \frac{ d n_{\gamma lm}(t) }{ dt }  = &     2 {  n_{a lm}  \over  \tau_a  } + \frac{ 16 \pi^2  }{ \beta m_a^3 \tau_a  } E_{l m }       \\ \nonumber
&   - \frac{ 16 \pi^2  }{ 3 m_a^3  \tau_a } (\beta+ {3\over2} )   F_{l m }
       -  \frac{3c}{2R}  n_{\gamma lm}(t)  ~,
\end{flalign}
where $E_{l m }$ and $F_{l m }$ are defined through
\begin{flalign} \label{elm}
n_a(\Omega, t)  n_{\gamma}(\Omega, t)   =&    \sum_{l'm'l'' m''}  n_{a l'm'}  n_{\gamma l'' m''}  Y_{l'm'} Y_{l''m''}   \\\nonumber
=&   \sum_{lm}  E_{l m } Y_{l m }
\end{flalign}
and
\begin{flalign} \label{flm}
[n_{\gamma}(\Omega, t)]^2  =& \sum_{l'm'l'' m''}  n_{\gamma l'm'}  n_{\gamma l'' m''}  Y_{l'm'} Y_{l''m''} \\\nonumber
=&   \sum_{lm}  F_{l m } Y_{l m }   ~.
\end{flalign}

We also have equations similar to equation \eqref{axioncoeff1} for each choice of $lm$  with regard to the changing number density of axions. The equation includes components representing spontaneous decay, stimulated decay and back reaction with sterile axions excluded
\begin{flalign} \label{axioncoeff2}
\frac{ d n_{a lm}(t) }{ dt }     &=   -  {  n_{a lm}  \over  \tau_a  }  -  \frac{ 8 \pi^2  }{ \beta m_a^3 \tau_a  } E_{l m }
                                                + \frac{ 8 \pi^2 \beta }{ 3 m_a^3  \tau_a }   F_{l m }    ~.
\end{flalign}
The sterile axions evolve according to
\begin{flalign} \label{saxioncoeff2}
\frac{ d n_{s lm}(t) }{ dt }     &=       \frac{ 4 \pi^2  }{  m_a^3  \tau_a }   F_{l m }    ~.
\end{flalign}
The rate of change of photon number density component can be expressed in terms of the changing components of normal axion and sterile axion, and the components of surface loss
\begin{flalign} \label{photoncoeff3}
 \frac{ d n_{\gamma lm}(t) }{ dt }  = &     -2 [ \frac{ d n_{a lm}(t) }{ dt }   + \frac{ d n_{s lm}(t) }{ dt } ]
       -  \frac{3c}{2R}  n_{\gamma lm}(t)  ~.
\end{flalign}

We now proceed to explore some example choices of initial axion distributions.

\section{Examples}
\subsection{$Y_{ 00 }$ distribution}
As a first example we consider the spherical symmetric axion distribution where
the only nonzero component of axion number density is $n_{a 00}$,
\begin{flalign} \nonumber
 n_a =& \Theta(R-r)   n_{a 00 }   Y_{ 00 }(\Omega)     ~,
\end{flalign}
then
\begin{flalign} \nonumber
 n_{a lm}=0  \quad(lm\neq00)  ~.
\end{flalign}
This simplifies equation \eqref{elm} to
\begin{flalign} \nonumber
n_a(\Omega, t)  n_{\gamma}(\Omega, t)       =  &      \sum_{lm}  n_{a 00} Y_{00}   n_{\gamma lm}  Y_{lm} ~.
\end{flalign}
In addition, there is now a relationship between $E_{lm}$ and $n_{\gamma lm}$,
\begin{flalign} \label{00-elm-photonlm}
E_{lm}=n_{a 00} Y_{00}   n_{\gamma lm}  ~.
\end{flalign}
Equation \eqref{axioncoeff2} is also simplified for $lm\neq00$ to
\begin{flalign} \nonumber
0    &=  0   -  \frac{ 8 \pi^2  }{ \beta m_a^3 \tau_a  } E_{l m }
                                                + \frac{ 8 \pi^2 \beta }{ 3 m_a^3  \tau_a }   F_{l m }     ~,
\end{flalign}
which reduces to
\begin{flalign} \label{00-elm-flm}
 F_{l m }  &=      \frac{ 3  }{ \beta^2    } E_{l m }     \quad(lm\neq00)  ~.
\end{flalign}
Substitute \eqref{00-elm-photonlm} and \eqref{00-elm-flm}  into equation \eqref{flm} gives, upon splitting of $00$ pieces, the two forms of  \eqref{flm}
\begin{flalign}
& [n_{\gamma}(\Omega, t)]^2      \label{00-ngng-1}
= F_{00} Y_{00} + \frac{ 3  }{ \beta^2    } n_{a 00} Y_{00}  \sum_{lm\neq00}  n_{\gamma l m } Y_{l m } \\ \nonumber
 F_{l m }  &=      \frac{ 3  }{ \beta^2    } E_{l m }     \quad(lm\neq00)  ~.
\end{flalign}
and
\begin{flalign}
& [n_{\gamma}(\Omega, t)]^2
= { n_{\gamma 00 } n_{\gamma 00 } \over 2\sqrt\pi}    Y_{00} +  2 n_{\gamma 00 }   Y_{00} \sum_{lm\neq00}  n_{\gamma l m } Y_{l m }     \nonumber \\
& + \sum_{l'm'l'' m'' \neq 0000}  n_{\gamma l'm'}  n_{\gamma l'' m''}  Y_{l'm'} Y_{l''m''}    ~.  \label{00-ngng-2}
\end{flalign}
The most conspicuous solution to the equation is
\begin{flalign} \nonumber
F_{00} ={ n_{\gamma 00 } n_{\gamma 00 } \over 2\sqrt\pi}     ~,\qquad
n_{\gamma lm}   =0 \quad(lm\neq00)  ~.
\end{flalign}
where the only nonzero component of photon number density is $n_{\gamma 00}$. So if there is spherical symmetry in the axion distribution, then spherical symmetry also exist in photon distribution.

Now we  argue that this is the only solution of finite spherical harmonics series. Suppose that the highest spherical harmonics in the photon number density $n_{\gamma}(\Omega, t)$ is $Y_{l_a m_a}$. According to \eqref{00-ngng-1} and taking the $Y_{00}$ as a number, the highest spherical harmonics in $ [n_{\gamma}(\Omega, t)]^2 $ is also $Y_{l_a m_a}$. However, according to \eqref{00-ngng-2}, the highest spherical harmonics in $ [n_{\gamma}(\Omega, t)]^2 $ is going to be $Y_{2l_a \, 2m_a}$. This contradiction can only be resolved when $n_{\gamma lm}   =0 \ (lm\neq00)$, i.e. the photon number density retains spherical symmetry.\\

The reason why this is the only finite series case is that the $Y_{00}$ distribution of axions mathematically requires the photons to couple in a specific way that retains the $Y_{00}$ distribution of axions, as is implied by equations \eqref{00-elm-photonlm} and \eqref{00-elm-flm}.

Now we know  all the coupling coefficients $E_{l m}$ and $F_{l m}$,
\begin{flalign} \nonumber
E_{l m}={ n_{a 00 } n_{\gamma 00 } \over 2\sqrt\pi} \delta_{l0}\delta_{m0}     ~,\qquad  F_{lm} ={ n_{\gamma 00 } n_{\gamma 00 } \over 2\sqrt\pi}  \delta_{l0}\delta_{m0}   ~.
\end{flalign}
Equations \eqref{photoncoeff2}, \eqref{axioncoeff2} and \eqref{saxioncoeff2}  reduce to the equations (34'), (37'), (38') in \cite{Kephart:1994uy} given that
\begin{flalign} \nonumber
n_{\gamma 00 } =  2\sqrt\pi  n_{\gamma  }     ~,\qquad  n_{a 00 } =  2\sqrt\pi  n_{a  }      ~,
\end{flalign}
because it is the $n_{\gamma 00 }Y_{00}$ that describes the photon number density. Hence we have checked the spherically symmetric model results given in  \cite{Kephart:1994uy} .

\subsection{$Y_{ 20 }$ distribution}
For a $Y_{ 20 }$ axion distribution the only nonzero component of the axion number density is $n_{a 20}$,
\begin{flalign} \nonumber
 n_a =& \Theta(R-r)   n_{a 20 }   Y_{ 20 }(\Omega)     ~,
\end{flalign}
so that
\begin{flalign} \nonumber
 n_{a lm}=0  \quad(lm\neq20)  ~.
\end{flalign}
Equation \eqref{axioncoeff2} is  simplified for $lm\neq20$, to
\begin{flalign} \nonumber
0    &=  0   -  \frac{ 8 \pi^2  }{ \beta m_a^3 \tau_a  } E_{l m }
                                                + \frac{ 8 \pi^2 \beta }{ 3 m_a^3  \tau_a }   F_{l m }     ~,
\end{flalign}
which reduces to
\begin{flalign} \label{20-elm-flm}
 F_{l m }  &=      \frac{ 3  }{ \beta^2    } E_{l m }     \quad(lm\neq20)  ~.
\end{flalign}
The  nonzero component $ n_{a 20}$ of axion number density evolves via
\begin{flalign}  \nonumber
\frac{ d n_{a 20}(t) }{ dt }     &=   -  {  n_{a 20}  \over  \tau_a  }  -  \frac{ 8 \pi^2  }{ \beta m_a^3 \tau_a  } E_{20}
                                                + \frac{ 8 \pi^2 \beta }{ 3 m_a^3  \tau_a }   F_{20}    ~.
\end{flalign}
The photon number density component $ n_{\gamma 20}$ growth rate is
\begin{flalign} \nonumber
 \frac{ d n_{\gamma 20}(t) }{ dt }  = &     2 {  n_{a 20}  \over  \tau_a  } + \frac{ 16 \pi^2  }{ \beta m_a^3 \tau_a  } E_{20}       \\ \nonumber
&   - \frac{ 16 \pi^2  }{ 3 m_a^3  \tau_a } (\beta+ {3\over2} )   F_{20 }
       -  \frac{3c}{2R}  n_{\gamma 20}(t)  ~,
\end{flalign}
while the other photon number density component $ n_{\gamma lm}(lm\neq20)$  evolve as
\begin{flalign} \nonumber
 \frac{ d n_{\gamma lm}(t) }{ dt }  =    - \frac{ 8 \pi^2  }{   m_a^3  \tau_a }     F_{lm }
       -  \frac{3c}{2R}  n_{\gamma lm}(t)  ~.
\end{flalign}
Since no spontaneous decay from axion feeds into these components, they are negligible. This example is not physical because a number density of the form $Y_{ 20 }$ becomes negative in some regions. It is included here for demonstration purpose. The next examples is physical and motivated by superradience.

\subsection{$  Y_1^{\pm1*} Y_1^{\pm1}\sim\sin^2\theta$ distribution}
A $sin^2\theta$ distribution is torodial  and is positive definite everywhere, and hence can represent a physical distribution of particles. For this case
the only nonzero components of the axion number density are $n_{a 00}$ and $n_{a 20}$,
so we can write $ n_a(r,\theta,t)$ in several useful forms
\begin{flalign} \nonumber
 n_a =& \Theta(R-r)   n_a(t)  \sin^2\theta       \\ \nonumber
=& \Theta(R-r)  n_a(t)  \frac{4\sqrt\pi}{3} ( Y_{00}-\frac{1}{\sqrt5}Y_{20})      \\ \nonumber
=&\Theta(R-r)  [ n_{a 00}(t)   Y_{00}  + n_{a 20}(t)   Y_{20} ] ~.
\end{flalign}
The relation between $n_{a 00}$ and $n_{a 20}$ is
\begin{flalign} \label{0020-axioncoeff}
   n_{a 20}(t)    =  - {  n_{a 00}(t)  \over \sqrt5 } ~.
\end{flalign}
 Similar to previous examples, we find that for components other than $00$ and $20$
\begin{flalign}  \nonumber
 F_{l m }  &=      \frac{ 3  }{ \beta^2    } E_{l m }     \quad(lm\neq00,20)  ~,
\end{flalign}
so that the components of photon number density evolve as
\begin{flalign} \nonumber
 \frac{ d n_{\gamma lm}(t) }{ dt }  =    - \frac{ 8 \pi^2  }{   m_a^3  \tau_a }     F_{lm }
       -  \frac{3c}{2R}  n_{\gamma lm}(t)  ~.
\end{flalign}\\

Since no spontaneous decay from axion feeds into these components, they are negligible, as  in the previous example. The nonzero axion number density components are given by
\begin{flalign}  \nonumber
\frac{ d n_{a 00}(t) }{ dt }   +  {  n_{a 00}  \over  \tau_a  }  &=     -  \frac{ 8 \pi^2  }{ \beta m_a^3 \tau_a  } E_{00}
                                                + \frac{ 8 \pi^2 \beta }{ 3 m_a^3  \tau_a }   F_{00}    \\  \nonumber
\frac{ d n_{a 20}(t) }{ dt }   + {  n_{a 20}  \over  \tau_a  }    &=   -  \frac{ 8 \pi^2  }{ \beta m_a^3 \tau_a  } E_{20}
                                                + \frac{ 8 \pi^2 \beta }{ 3 m_a^3  \tau_a }   F_{20}    ~.
\end{flalign}
Because of \eqref{0020-axioncoeff}, this leads to the relation
\begin{flalign}  \nonumber
&-  \frac{ 8 \pi^2  }{ \beta m_a^3 \tau_a  } E_{20}  + \frac{ 8 \pi^2 \beta }{ 3 m_a^3  \tau_a }   F_{20}     \\  \label{0020-elm-flm}
=&       {1\over\sqrt5}    (  \frac{ 8 \pi^2  }{ \beta m_a^3 \tau_a  } E_{00}  -  \frac{ 8 \pi^2 \beta }{ 3 m_a^3  \tau_a }   F_{00}   )       .
\end{flalign}
The photon number density component $ n_{\gamma 20}$ grows as
\begin{flalign} \nonumber
 \frac{ d n_{\gamma 00}(t) }{ dt }  = &     2 {  n_{a 00}  \over  \tau_a  } + \frac{ 16 \pi^2  }{ \beta m_a^3 \tau_a  } E_{00}       \\ \nonumber
&   - \frac{ 16 \pi^2  }{ 3 m_a^3  \tau_a } (\beta+ {3\over2} )   F_{00 }
       -  \frac{3c}{2R}  n_{\gamma 00}(t)   \\ \nonumber
       \end{flalign}
       and
       \begin{flalign} \nonumber
 \frac{ d n_{\gamma 20}(t) }{ dt }  = &     2 {  n_{a 20}  \over  \tau_a  } + \frac{ 16 \pi^2  }{ \beta m_a^3 \tau_a  } E_{20}       \\ \nonumber
&   - \frac{ 16 \pi^2  }{ 3 m_a^3  \tau_a } (\beta+ {3\over2} )   F_{20 }
       -  \frac{3c}{2R}  n_{\gamma 20}(t)  ~.
\end{flalign}
Because of \eqref{0020-axioncoeff} and \eqref{0020-elm-flm}, we can combine the previous two equations and write
\begin{flalign} \nonumber
& \frac{ d n_{\gamma 00}(t) }{ dt }  + \frac{3c}{2R}  n_{\gamma 00}(t)   \\ \nonumber
  = &     2 {  n_{a 00}  \over  \tau_a  } + \frac{ 16 \pi^2  }{ \beta m_a^3 \tau_a  } E_{00}         - \frac{ 16 \pi^2  }{ 3 m_a^3  \tau_a } (\beta+ {3\over2} )   F_{00 }       ~,     \\ \nonumber
& \frac{ d n_{\gamma 20}(t) }{ dt }  + \frac{3c}{2R}  n_{\gamma 20}(t)   \\ \nonumber
= &     2 {  n_{a 00}  \over  \tau_a  } ({-1\over\sqrt5}) +  (\frac{ 16 \pi^2  }{ \beta m_a^3 \tau_a  } E_{00}         - \frac{ 16 \pi^2  \beta }{ 3 m_a^3  \tau_a }   F_{00 }   )   ({-1\over\sqrt5})  \\ \nonumber
  & - \frac{ 8 \pi^2  }{  m_a^3  \tau_a }     F_{20 }   \\ \nonumber
= &    {-1\over\sqrt5}  [ \frac{ d n_{\gamma 00}(t) }{ dt }  + \frac{3c}{2R}  n_{\gamma 00}(t) ]  - \frac{ 8 \pi^2  }{  m_a^3  \tau_a }     F_{20 }
\end{flalign}
We observe that if the part of back reaction that results in sterile axions is neglected, then
\begin{flalign} \nonumber n_{\gamma 20}(t)    =  - {  n_{\gamma 00}(t)  \over \sqrt5 }   ~, \end{flalign}
so the photons would remain in $\sin^2\theta$ distribution.\\

\subsection{General distribution}
Suppose that we have an axion number density
\begin{flalign} \nonumber
 n_a =& \Theta(R-r)  \sum    n_{a l m }   Y_{ l m }(\Omega)     ~,
\end{flalign}

For $n_{a l m } = 0$, then according to \eqref{axioncoeff2} this leads to
\begin{flalign} \nonumber
F_{lm} =& { 3 \over \beta^2 }  E_{lm}  ~~  ( n_{a l m } = 0 )
\end{flalign}
Substituting this condition into equation \eqref{photoncoeff2}, we have
\begin{flalign} \nonumber
 \frac{ d n_{\gamma lm}(t) }{ dt }  = &         - \frac{ 16 \pi^2  }{ 3 m_a^3  \tau_a } ( {3\over2} )   F_{l m }
       -  \frac{3c}{2R}  n_{\gamma lm}(t)
\end{flalign}
also for  $n_{a l m } = 0$.
Hence there is no source feeding those photon components.

The parts of back reaction that results in sterile axions and surface loss are the only terms that contribute to these components. It is expected that these components die out quickly and thus have no effect on lasing. So
\begin{flalign} \nonumber
n_{\gamma} =  \,    & \Theta(R-r)  \sum   n_{\gamma l m  }   Y_{ l  m }(\Omega)     ~.
\end{flalign}
where
\begin{flalign} \nonumber
n_{\gamma l m } \approx   0   ~~  ( \text{when } n_{a l m } = 0 ) ~.
\end{flalign}
I.e., the photon field has the same spherical harmonic components as the axion field, as other components  die out quickly due to lack of sources. Neither spontaneous decay nor stimulated decay contributes to the harmonic components of photons that are not present in the axions.

Suppose that all the axion components are nonzero, and they are proportional to each other,
$$n_{a l  m } = \alpha_{lm} n_{a l_0 m_0 } ,$$  where $\alpha_{lm}$ are numbers and $n_{a l_0 m_0 }$ is the fiducial component to which all other components are proportional. Then
\begin{flalign} \nonumber
\frac{ 8 \pi^2 \beta }{ 3 m_a^3  \tau_a }   F_{ lm }   -  \frac{ 8 \pi^2  }{ \beta m_a^3 \tau_a  } E_{ lm }  =    \frac{ d n_{a lm }(t) }{ dt }     +    {  n_{a lm  }  \over  \tau_a  }          \\ \nonumber
\end{flalign}
and
\begin{flalign} \nonumber
& \frac{ d n_{\gamma  lm }(t) }{ dt } +   \frac{3c}{2R}  n_{\gamma  lm  }(t)           \\ \nonumber
= &     2 {  n_{a   lm  }  \over  \tau_a  } + \frac{ 16 \pi^2  }{ \beta m_a^3 \tau_a  } E_{  lm  }
          - \frac{ 16 \pi^2  }{ 3 m_a^3  \tau_a } (\beta+ {3\over2} )   F_{   lm   }      \\ \nonumber
=&    -2  \frac{ d n_{a  lm }(t) }{ dt }  - \frac{ 8 \pi^2  }{  m_a^3  \tau_a }     F_{   lm }
\end{flalign}
If the part of the back reaction that results in sterile axions is neglected, then
\begin{flalign} \nonumber
& \frac{ d n_{\gamma  lm  }(t) }{ dt } +   \frac{3c}{2R}  n_{\gamma  lm  }(t)           \\ \nonumber
=&    -2  \frac{ d n_{a  lm  }(t) }{ dt }   =   -2  \alpha_{ lm } \frac{ d n_{a  l_0 m_0 }(t) }{ dt }    \\ \nonumber
=& \alpha_{ lm }  [   \frac{ d n_{\gamma  l_0 m_0 }(t) }{ dt } +   \frac{3c}{2R}  n_{\gamma  l_0 m_0 }(t)   ]
\end{flalign}
\begin{flalign} \nonumber
n_{\gamma   lm }= \alpha_{ lm }  n_{\gamma  l_0 m_0 }   \end{flalign}
Hence the distribution of photons would keep the same shape as that of the axions if sterile axions were neglected.\\

\section{Discussion}
The calculation presented here tells one the initial spatial distribution of photons once the spatial distribution of the axions is given. It does not give direct instructions on how to achieve observable effects from axion cluster lasing. The model does take the mechanism that the stimulated decay of axion produces type of photons that have the same momenta as the photons which induced the stimulated decay process.
\begin{flalign} \nonumber
 2k \frac{d f_\lambda ( \vec{k} )  }{dt}  =&  \frac{4 m_{a} \Gamma_{a} }{ \pi }  \int \frac{d^3  k_1   }{ 2k_1^0 } \frac{d^3  p   }{ 2p^0 }  \delta^4 (p-k-k_1) \times \\  \nonumber
   &  \{  f_a  ( \vec{p} ) [ 1+ f_\lambda ( \vec{k} ) + f_\lambda ( \vec{k}_1 ) ] - f_\lambda ( \vec{k} )f_\lambda ( \vec{k}_1 ) \}  ~.
\end{flalign}
However, there is a compromise made here by using this equation. The entire model is a local theory. The photon occupation number here and now depends only on particle occupation numbers here and now. If the cluster in the model is a ball and all the quantities are spherical symmetric, the local theory provides useful predictions about the lasing process. However, if the cluster is of some specific geometrical shape, then the local theory probably won't give pertinent information that reflect the geometry of the cluster. Thus we suggest that a non-local lasing theory which could be governed by the following equation,
\begin{flalign} \nonumber
 & 2k \frac{d f_\lambda ( \vec{k} ,\vec{x}, t )  }{dt} =   \frac{4 m_{a} \Gamma_{a} }{ \pi }  \int \frac{d^3  k_1   }{ 2k_1^0 } \frac{d^3  p   }{ 2p^0 }  \delta^4 (p-k-k_1)   \\  \nonumber
& \times  C \int d^3x' \{  f_a  ( \vec{p} ,\vec{x}', t' )   \int^t dt' e^{- \Gamma_{a}(t-t')} \delta[\vec{x} - \vec{x}' - {c\vec{k} \over k} (t-t')]    \\  \nonumber
   &+ f_a  ( \vec{p} ,\vec{x}, t )  \int^t dt' e^{- \Gamma_{a}(t-t')} \delta[\vec{x} - \vec{x}' - {c\vec{k} \over k} (t-t')]
  f_\lambda ( \vec{k} ,\vec{x}' ,t' )    \\  \nonumber
& +f_a  ( \vec{p} ,\vec{x}, t )   \int^t dt' e^{- \Gamma_{a}(t-t')} \delta[\vec{x} - \vec{x}' - {c\vec{k}_1 \over k_1} (t-t') ]
  f_\lambda ( \vec{k}_1 ,\vec{x}' ,t' )    \\  \nonumber
&- f_\lambda ( \vec{k} ,\vec{x}, t   )   \int^t dt' e^{- \Gamma_{a}(t-t')} \delta[\vec{x} - \vec{x}' - {c\vec{k}_1 \over k_1} (t-t')]
f_\lambda ( \vec{k}_1 ,\vec{x}' ,t' ) \} ~.
\end{flalign}
In the non-local model, the photon occupation number here and now depends on all the past occupation number of events that are casually connected to here and now.
The factor $e^{- \Gamma_{a}(t-t')}$ takes account the probability that photons propagating from $\vec{x}' $ to $\vec{x}$ without stimulating axion or going to annihilation.
\section{Appendix}
Starting from the  evolution relation between axion and photon occupation numbers \cite{Kephart:1994uy}
\begin{flalign} \label{13Kephart}
&\frac{d f_\lambda ( k )  }{dt} =\frac{m_a \Gamma_a}{k^2} \int_{\frac{m_a^2}{4k}} d k_1     \\ \nonumber
&\times \{  f_a  ( k+k_1 ) [ 1+ f_\lambda ( k ) + f_\lambda ( k_1 ) ] - f_\lambda ( k )f_\lambda ( k_1 ) \}
\end{flalign}
where $f_\lambda ( k )$ and $f_\lambda ( k_1 )$ are photon  occupation numbers of momentum $k$ and $k_1$, respectively. Other variables in $f_\lambda ( k )$ and $f_\lambda ( k_1 )$, i.e. $r, \theta, t$, are the same since they share the same spacetime. $ f_a  ( k+k_1 ) $ is the axion occupation number of momentum $k+k_1$. $\Gamma_a$ is the spontaneous axion decay rate. Substitute \eqref{axionON} and \eqref{photonON} into \eqref{13Kephart} we arrive at
\begin{flalign}\nonumber
&\frac{d f_\lambda ( k )  }{dt} =\frac{m_a \Gamma_a}{k^2}  \bigg\{ [ 1+ f_\lambda ( k ) ]  f_{ac} \, \Theta(R-r)  X(\theta)  &&\\ \nonumber
&\quad \times \int_{\frac{m_a^2}{4k}} \Theta(p_{\textrm{\tiny max}}-\sqrt{(k+k_1)^2-m_a^2}) d k_1  &&\\ \nonumber
&\quad +f_{ac} f_{\lambda c} \, [\Theta(R-r)]^2  X(\theta) \, Y(\theta)  \,\times&&\\ \nonumber
&\int_{\frac{m_a^2}{4k}} \Theta( p_{\textrm{\tiny max}}-\sqrt{(k+k_1)^2-m_a^2})\Theta(k_+-k_1) \Theta(k_1-k_-) d k_1  &&\\ \nonumber
&-f_\lambda(k)  f_{\lambda c} \Theta(R-r) \, Y(\theta)  \int_{\frac{m_a^2}{4k}} \Theta(k_+-k_1) \Theta(k_1-k_-) d k_1
\bigg\}  ~.
\end{flalign}
The first and second  integrals are the same,
\begin{flalign} \nonumber
&\quad  \int_{\frac{m_a^2}{4k}} \Theta(p_{\textrm{\tiny max}}-\sqrt{(k+k_1)^2-m_a^2}) d k_1  \\ \nonumber
&=\int_{\frac{m_a^2}{4k}} \Theta( p_{\textrm{\tiny max}}-\sqrt{(k+k_1)^2-m_a^2})\Theta(k_+-k_1) \Theta(k_1-k_-) d k_1
\\ \nonumber
&=m_a\gamma-k-\frac{m_a^2}{4k} ~.
\end{flalign}
The third integral is related to the back reaction of photons. It is convenient to split it into two parts
\begin{flalign} \nonumber
&\quad  \int_{\frac{m_a^2}{4k}} \Theta(k_+-k_1) \Theta(k_1-k_-) d k_1     \\ \nonumber
&=\int_{\frac{m_a^2}{4k}}^{m_a\gamma-k} d k_1 + \int_{m_a\gamma-k}^{k_+}   d k_1  \\ \nonumber
&= (m_a\gamma-k-\frac{m_a^2}{4k} ) +  (k-k_-)    ~.
\end{flalign}
The first part represents back reaction resulting in axions with energy a  less than $m_a\gamma$ that  axions that can again participate in stimulated emission, while the second part gives the back reaction resulting in sterile axions, i.e., where the total energy of the axion $k+k_1$ is larger than $m_a\gamma$.

Moving the step function $\Theta(R-r)$ in front of the  curly brackets and substituting the results of the integrations, we have
\begin{flalign} \nonumber
 \frac{d f_\lambda ( k )  }{dt} &=  \Theta(R-r) \, \frac{m_a \Gamma_a}{k^2}  \bigg\{   &&\\ \nonumber
&\quad [ 1+ f_\lambda ( k ) ]  f_{ac} \, X(\theta) \, (m_a\gamma-k-\frac{m_a^2}{4k} )  &&\\ \nonumber
&\quad + f_{ac} f_{\lambda c} \,  X(\theta)  \, Y(\theta) \, (m_a\gamma-k-\frac{m_a^2}{4k} ) &&\\ \nonumber
&\quad -f_\lambda(k) f_{\lambda c}  Y(\theta) \, [ (m_a\gamma-k-\frac{m_a^2}{4k} ) +  (k-k_-) ]   \bigg\}.
\end{flalign}
Collecting  terms $f_\lambda(k)$ can be written
\begin{flalign} \nonumber
\frac{d f_\lambda ( k )  }{dt} &= \Theta(R-r) \Theta(k_+-k) \Theta(k-k_-) \, \frac{m_a \Gamma_a}{k^2}  \bigg\{   &&\\ \nonumber
&\qquad [f_{ac} ( X + 2f_{\lambda c} \, XY    ) -f_{\lambda c}^2  Y^2 ] (m_a\gamma-k-\frac{m_a^2}{4k} )  &&\\  \nonumber
&\qquad -f_{\lambda c}^2  y^2  (k-k_-)
\bigg\}  ~.
\end{flalign}
The rate of change of photon number density is the integration of this equation over $k$ space
\begin{flalign} \nonumber
\frac{d n_\lambda  }{dt}  &= \int \frac{d f_\lambda ( k )  }{dt} \frac{d^3k}{(2\pi)^3}   &&\\ \nonumber
&= \Theta(R-r)  \frac{m_a \Gamma_a}{ 2\pi^2 } \bigg\{    [f_{ac} ( X + 2f_{\lambda c} \, XY    ) -f_{\lambda c}^2  Y^2 ]   \times &&\\ \nonumber
&\quad \int_{k_-}^{k_+} (m_a\gamma-k-\frac{m_a^2}{4k} ) dk - f_{\lambda c}^2  y^2  \int_{k_-}^{k_+}  (k-k_-) dk \bigg\}
\end{flalign}
Evaluating the two integrals,
\begin{flalign} \nonumber
 & \int_{k_-}^{k_+} (m_a\gamma-k-\frac{m_a^2}{4k} ) dk
= \frac{m_a^2\gamma^2\beta}{2}  -\frac{m_a^2}{4}\ln\bigg( \frac{1+\beta}{1-\beta} \bigg)   \\ \nonumber
& \int_{k_-}^{k_+}  (k-k_-) dk = \frac{m_a^2\gamma^2\beta^2}{2}   ~.
\end{flalign}
gives
\begin{flalign} \nonumber
\frac{d n_\lambda  }{dt}
&= \Theta(R-r)  \frac{m_a^3 \Gamma_a}{ 8\pi^2 } \bigg\{    [f_{ac} ( x + 2f_{\lambda c} \, xy    ) -f_{\lambda c}^2  y^2 ]   \times &&\\ \nonumber
&\quad [2\gamma^2\beta -\ln\bigg( \frac{1+\beta}{1-\beta} \bigg) ] - f_{\lambda c}^2  y^2 \times (2 \gamma^2\beta^2    ) \bigg\}
\end{flalign}

\vfill

\vspace{0.2cm}
\begin{acknowledgments}

\end{acknowledgments}

\vfill

redpajama_set_name: RedPajamaArXiv


text:
package org.spincast.core.server;

/**
 * Some utilities for server implementation.
 */
public interface ServerUtils {

    /**
     * This must be called by a {@link Server}
     * implementation, after it has been successfully
     * started!
     *
     */
    public void callServerStartedListeners();

}

redpajama_set_name: RedPajamaGithub


text:
Things to Do with Kids in Kingsport, TN
TripBuzz found 58 things to do with kids in or near Kingsport, Tennessee, including 43 fun activities for kids in nearby cities within 25 miles like Johnson City, Bristol, Jonesborough and Bristol.
From Putt-Putt Fun Center to Kingsport Aquatic Center, the Kingsport area offers 47 different types of family activities, including: Movie Theaters, Golf, Bowling and Family Fun Center.
Kingsport, Tennessee spans Sullivan, Hawkins, and Washington counties and maintains a large population of nearly 50,000 residents. The area is settled in the Mountain Empire of eastern Tennessee, making for a varied and scenic terrain. The adjacent Holston River, providing for even more opportunities for outdoor adventure, accentuates the areas natural beauty.
Winter Activities (3)
History Museums (4)
National & State Parks (3)
Historic Homes (2)
Race Car Driving (1)
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Dance Studios (1)
Nature & Wildlife Areas (1)
Other Tours (1)
Indoors (46)
Johnson City (17)
Kingsport (15)
Greeneville (14)
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Putt-Putt Fun Center
Family Fun Center 346 W Stone Drive, Kingsport, TN 37664 MoreLess Info
Enjoy the classic 18-hole family outing at Putt Putt Fun Center in Kingsport. Putt Putt is an ideal place for a fun-filled date night or for your child's next birthday party.
Kingsport Aquatic Center
Water Parks 1820 Meadowview Parkway, Kingsport, TN 37660 MoreLess Info
An indoor and outdoor swimming and recreation center, The Kingsport Aquatic Center features an indoor Olympic size pool and an outdoor water park and play area. The center also offers swimming lessons.
Warrior's Path Riding Stables
Horseback Riding 1882 Fall Creek Road, Kingsport, TN 37664 MoreLess Info
Situated inside the state park of the same name, Warrior's Path Riding Stables specializes in trail riding and guided tours of varying length on weekends from spring through fall. The stable also offers a boarding service as well.
Warpath Bowling Lanes
Bowling 2449 Memorial Blvd, Kingsport, TN MoreLess Info
Warpath Bowling Lanes offers bowling on AMF HPL Glow-Track synthetic lanes with 82-90XL AMF pinsetters. The facility offers glow-in-the-dark bowling at certain times, along with open and league bowling for all ages.
Warriors' Path State Park
National & State Parks Hemlock Road, Kingsport, TN MoreLess Info
The most popular activities at Warriors' Path State Park in Kingsport, Tennessee include hiking, mountain biking, fishing, boating and relaxing in the shade. The park also features a large campground, for which reservations are recommended.
Exchange Place
Farms & Ranches 4812 Orebank Road, Kingsport, TN MoreLess Info
Kingspot, Tennessee's Exchange Place is a volunteer-run historical interpretive center that lets guests experience Appalachian life during the turn of the 20th century. Exchange Place is open from May to October and hosts several popular annual fairs and conventions.
Kingsport Speedway
Race Tracks 2962 N John B. Dennis Hwy, Kingsport, TN 37660 MoreLess Info
Featuring a 3/8th mile oval track, Kingsport Speedway showcases NASCAR and stock racing during its racing season, which begins in March and ends in September. The speedway has a kid's club where children can experience racing related activities.
Parks 2201 Netherland Inn Rd, Kingsport, TN 37664 MoreLess Info
Kingsport's Riverfront Park, often called the Boatyard-Riverfront Park, is a municipal park. It has two trails, flush bathrooms, two reservable canopied picnic spots and a large playground. Fishing is permitted from the docks.
Marquee Cinemas
Movie Theaters 2101 Fort Henry Dr, Kingsport, TN 37664 MoreLess Info
Indulge your love of a good movie at Marquee Cinemas in Kingsport, Tennessee. Part of the Marquee theater chain, this location screens new releases and occasionally hosts re-releases of classic films. It is also available for corporate meeting rentals.
Movie Theaters 2101 Fort Henry Drive, #71, Kingsport, TN 37664 MoreLess Info
At Frank Theatres Kingsport Town Center, visitors can see the latest films in standard and 3D viewing formats. The concession offers popcorn buckets which can be refilled at a discounted price.
HAVE SUGGESTIONS FOR COOL AND INTERESTING THINGS TO DO IN THE Kingsport AREA?


text:
Universal Jurisdiction Tools
Universal jurisdiction database
What does TRIAL International do in Bosnia and Herzegovina?
Local structure
In the 1990s, war ravaged the former Yugoslavia. Bosnia and Herzegovina was particularly affected from 1992 to 1995, and although hostilities ceased several decades ago, the consequences are still felt today. In this post-war context, TRIAL International prioritizes advocacy and judicial capacity building for victims to invoke their rights.
The break-up of Yugoslavia triggered numerous mass crimes in Bosnia and Herzegovina: genocide, war crimes, enforced disappearances, sexual violence, etc. It also caused the death of nearly 100'000 people.
Despite the establishment of an international tribunal (the ICTY, which closed in 2017) and numerous trials at a national level, many victims are still waiting for justice. Some criminals go unpunished, and even convictions do not always result in reparations for victims.
The Bosnian authorities constantly evoke the need to move on and forget the atrocities of war, but by adopting this attitude they neglect the rights and needs of many survivors.
TRIAL International has been working on Bosnia and Herzegovina since 2008. Its support first consisted of free legal assistance to victims of the war. It has achieved great victories before national courts and international bodies. New cases are now rarer, but the organization continues to support some of its earliest beneficiaries, simply because they still have rights to invoke – including the right to receive reparations for their sufferings.
By insisting on the need to put the war behind, authorities neglect the rights and needs of many survivors.© Olja Latinovic
Advocating for greater justice
To be compelling, the legal battle before courts and other jurisdictions must go hand in hand with long-term advocacy. In BiH, TRIAL International calls on the authorities to put into practice court rulings in favor of victims of serious crimes and to align their national legislation with international standards. In association with partner NGOs, TRIAL informs the international community about serious human rights violations taking place in the country, so that they can measure the urgent need for action.
Aligning Bosnian law with international standards
Today, TRIAL International focuses more on structural amendments to Bosnian law. It calls on the authorities to align national legislation with international human rights, such as access to reparations for victims of sexual violence. For example, in August 2019, the United Nations Committee Against Torture condemned the Bosnian authorities and ordered them to make reparations to a rape victim.
In addition, TRIAL International seeks to publicize its successes among legal professionals. A single precedent can thereby become a practice extended to the whole country. This is particularly important in view of the many political and jurisdictional levels in Bosnia and Herzegovina, which too often result in "double standards" for victims depending on where they live.
For this purpose, TRIAL International regularly organizes training for prosecutors, lawyers and judges. It also publishes legal guides to their intention.
TRIAL opened an office in Sarajevo, the capital of Bosnia and Herzegovina, in 2011. Since then, its Bosnian staff have been working in an office located at 19 Čobanija in Sarajevo.
Legislation Pertaining to Children Born of War in Bosnia and Herzegovina: A Resounding ...
On 14 July 2022, Brčko District of Bosnia and Herzegovina (BDBiH) passed a law on civilian victims of war, wi...
[🔈PODCAST] Fighting wartime sexual violence: lessons from Bosnia and DRC
In Bosnia and Herzegovina, in the Democratic Republic of the Congo, and during so many other conflicts, sexual violence...
Double jeopardy for wartime torture victims of Bosnia and Herzegovina: After having the...
Victims of war crimes are now victims of failed reparations mechanism Sarajevo and Geneva, 26th of September – A growin...
Children born as a result of wartime rape get their first legal recognition in Bosnia a...
Sarajevo, 2 August 2022 - After years of struggle to obtain recognition of their existence and their status, a...
International Day for the Elimination of Conflict Related Sexual Violence : "We are not...
Stronger than crime: "We are not victims, we are survivors!" For the International Day for the Elimination of Sexual Vi...
Bosnia and Herzegovina : 30 years since the beginning of the war, survivors of conflict...
"It took me a long time to get my voice, now that I have it, I won't keep quiet" Survivor of conflict-related sexual v...
The fight for justice knows no borders: 29 years after war crimes were committed in Foč...
Slobodan Curcic, who is suspected of having committed war crimes in Foča (Bosnia and Herzegovina - BiH) in 1992, includi...
« Now he is a convicted criminal, I transferred my burden to him. You are the victim no...
Words from Semka Agic, survivor of conflict-related sexual violence More than 20,000 women and men were raped...
Denying wartime horrors is now a criminal offence in BiH
Denial of genocide and other war crimes, that is likely to incite violence or hatred, is now prohibited by law in Bosnia...
Will Mladić's conviction be enough to silence denial in BiH?
While Ratko Mladić's sentence to life imprisonment has just been confirmed, revisionist and genocide denial discourse is...
Compensation to war crimes victims in BiH, a matter of willingness
Compensation for victims of war crimes is possible, as four recent examples in Bosnia and Herzegovina (BiH) have shown....
Sexual violence in BiH: A new step forward in the right direction
Since March 2021, the Criminal Procedure Code of the Republika Srpska prohibits presenting evidence of the victim's sexu...
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Nothing to worry about : your host family will come and pick you up at the station (Reims-Centre or Champagne-Ardennes TGV) They will welcome you with an apéritif, and help you with your new environment.
Studying in France will have you discover French cuisine: you will love it ! You will be able to cook your own meals in your host family. Your host will have cabinet and refrigerator space available for you to store your foods. You will make arrangements for sharing the kitchen with your hosts. Lunch may be taken on campus or in town.
You might choose to share a few meals with your hosts (1 or 2 per week, for an extra fee of 30€ or 60€ per month) A good opportunity to experience nice French family meals and practice your French !
Do not miss our welcome apéritif at the start of your stay !


Rooster Booster Poultry Booster, 1.25 lb. at Tractor Supply Co.
Rooster Booster Poultry Booster is a pelleted top dress vitamin and mineral supplement for all classes of poultry and fowl. Use Rooster Booster Poultry Booster on all ages of poultry and fowl for growth, development and egg production programs. Also contains all the vitamins, minerals and amino acids necessary for healthy, happy adult fowl including laying hens.
Package Size: 1.25 fl. oz.
Rooster Booster Poultry Booster, 1.25 lb. is rated 4.6 out of 5 by 11.
Rated 5 out of 5 by Pammygirl57 from Happy and healthy I believe my ladies benefited from that first jar I bought. I plan to get another and keep them happy and healthy.
Rated 5 out of 5 by Popcorn444 from My Chickens LOVE this I am so glad to have found this product. Chickens love it. When I add this to their feed they are more content, satisfied, and eat less.
Rated 5 out of 5 by BeccaBwithbirds from Great supplement for broody hens! Had some broody Silkie hens that weren't getting proper nutrition, gave 1cc orally and mixed with water. They perked right up!
can a chicken OD on this stuff? Mine are scattering their food to the 4 winds trying to find all of this stuff that was mixed in. Will they get sick if they eat too much?
They will not get sick if they eat too much. Long term there may be minor issues from excess calcium. When introducing this to birds, they tend to pick it out and eat it exclusively while trying to get their proper nutrients. As long as you stick to the recommended 1 scoop per 3 birds, it will be fine.


text:
Tag: Draw day
PTA fails to keep people informed about banned and unbanned websites
PTA Updates Page Snapshot
It is 30th may today and the last update on PTA's website about the blocked websites was on 2oth of may. They even didn't even mentioned any other blocked websites other than the Facebook and Youtube on their website. Hundreds of URLs were blocked and some of websites like Facebook , wikipedia, youtube and many more had faced blanket ban but PTA never mentioned about these banned websites on their website.
Youtube is already unblocked few days ago but still no update about that on their website. Whats more important is Pakistan Telecommunication Authority (PTA) never published the details of blocked websites over the internet nor they have updated people about when certain websites are being banned or unbanned. It would have been much better if things would have been much more transparent.
Proxy websites blocked in Pakistan, Whats the point?
In connection with the issue of blasphemous violent content, Pakistan Telecommunication Authority (PTA) blocked many websites and many people including me supported this decision of PTA. Banning the websites in Pakistan should have not mainly to prevent local people from accessing the blasphemous content but to make a statement to sites that your racism regarding the religion will not be accepted.
Considering the fact that Pakistan is an Islamic state and people at least have love for prophet Muhammad, no one would be willing to see that blasphemous content. But unfortunately PTA took things here differently, they gone few steps further and also blocked the proxy website.
Chairman PTA: We have blocked a number of sites having the blasphemous content and also blocked some proxy websites, so that the content can't be accessed in Pakistan in anyway.
Blocking the original websites was more than enough to make a statement and blocking the proxy websites was unnecessary step. Ideally no one would try to access that blasphemous content via proxies, at least those who follow Islam and love Prophet Muhammad (PBUH) and if some one would, well every one is responsible for his/her own faith.
In fact the guys blocking the proxy websites didn't thought about the positive features and capabilities which proxies enable us with, they only kept eye on negativity and end up blocking most of proxy websites known to them.
At times proxy websites are very useful, some times certain ISP dns servers don't have most updated IP records against domains or have problems with certain websites, in this case the proxy websites are the only handy tool to access them.
Finally I would say, it would have been better, if ban must have been symbolic for the world other than just to restrict the locals from looking at the content. Whatever else is done, I am in full favor of that but not in favor of blocking the proxy websites which still are blocked in Pakistan.
Ban on Facebook in Pakistan, right or wrong?
One would say why are we even talking about the ban being right or wrong when Facebook proved to be racist in matter of removing the draw day. Making one thing clear here, Facebook guys remove any page with more than 10,000 fans on just 700 terms of use violation requests against it, but this was not the case about the page which was setup to hold that blasphemes cartoons contest.
Coming back to the original topic, why are we even thinking on the ban being right or wrong, most would say it right because of the Facebook's resist behavior in this matter. But there are people who are not in support of this ban, they think that the URLs where such kind of content is added must be blocked but not the whole Facebook site. Well for their information the ban is not here to prevent the people of Pakistan from seeing such kind of content – which they will not see even is not blocked – the ban is here in the first place to send a message to Facebook or any such websites that if you will come up with any resist behavior for us, we then do not need to even use your sites, can live very much without them.
There are people who were in favor of Ban on Facebook from day one, they speaked out many different ways, some recorded their protest via online posts and tweets and there were others who came in with peaceful protests on they city roads of all major cities and towns of Pakistan. This all led to the Ban order on Facebook by Lahore High Court, which is implemented countrywide for good.
What we have discussed above is the first extreme, now there are other people from Pakistan who are completely against the ban. Well they are not only against the ban, some of them have officially got recorded their protest against the ban and speaked up against it. One such example is this press conference against the ban on Facebook in Pakistan which appeared on Awab Alvi's blog who is a well known and popular blogger from Pakistan.
Awab Alvi: While we recognize that sites on the Internet are used to spew hatred and incite violence, we steadfastly believe that governments have no right to control access to information. We believe that every citizen has an inalienable right to freely access information and by censoring Facebook, the Government of Pakistan has taken away that right
Well I will second that opinion, this time the demand for ban was initiated from the people of Pakistan, not from the government or the judiciary of Pakistan. Most of Pakistanis still stand by this decision and hope for a ban until Facebook realizes that they are doing something which is not liked by billions of people worldwide and that is the racism which came forward in matter of Draw day.
I have listened people saying where Facebook have 400 million users from world wide how stopping access of just 2 million or so users from Pakistan is going to hurt Facebook. First thing we are making it clear to the world that no such religious racism will be tolerated by Pakistanis and secondly its definitely going to hurt Facebook if they are to continue such dual behavior. Facebook is ranked two in world websites ranking and the fight for the number one slot is on, such behaviors are cost Facebook to be pushed back to number three or four instead of making it to the number one slot.
Finally we will boycott any website which shows the tolerance for the content which hurts the feelings of believers of any religion. Religion is the personal matter of any being living on planet earth and if you are heating the feelings of believers of any religion, weather its Islam or any other religion, you have no right to be called a civilized human being and nations who show tolerances for such content are not civilized nations at all.
Do write your views about the decision of banning Facebook in Pakistan below as comments and whether you are in favor of that decision or not. Feel free to express your views. Subscribe to our Twitter page and update emails from sidebar to keep yourself updated on latest information.


What presence is detected in Presence Mode?
Discussion in 'XeThru Explorer' started by Peter Prodinger, Jul 2, 2015.
i would like to know, if the Presence mode from the current XeThru Explorer is set to detect any kind of movement or does it work together with the Respiration mode to detect only "human" presence.
Both modes will detect any kind of movement that is perceived as "strong enough". The respiration mode has the additional capability to distinguish between any kind of movement and a person's breathing pattern.
That was exactly the answer i was looking for.


Several new pieces, from various shows.
Since I'm leaving for California on Sunday I wanted to let you know that if you've been thinking about buying anything from my store do it now! Orders placed before Friday will go into the mail before I leave, otherwise I won't be shipping until after May 30th. Until then order away!


This entry was posted on Saturday, August 23rd, 2014 at 2:14 pm and is filed under Anticonformismo e pensieri.	You can follow any responses to this entry through the RSS 2.0 feed. Both comments and pings are currently closed.


text:
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Gustavus Class of 2010
Orthopedic Surgical Resident, University of Minnesota
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Life of Service
T.J. Ridley has taken the idea of leading a life of purpose to heart. This concept, the cornerstone of so much of a Gustie's four years on campus, has directed him to a career where he serves others on a daily basis. "For me, that purpose is improving or enriching the lives of others," he says. "To maintain focus through school and training, it has been important that I not only love what I do, but truly enjoy serving and treating others."
T.J. was attracted to Gustavus because he could participate in rigorous academics as well as competitively play not one but two sports: hockey and football. His pre-med biology major led him to his current position as an orthopaedic surgeon at the University of Minnesota. His sports career garnered numerous accolades, including being named twice to the College Sports Information Directors of America (CoSIDA) Academic All-America Team, a semifinalist for the National Football Foundation's William V. Campbell Trophy, and winning the College Football Hall of Fame National Scholar Athlete Award.
"Gustavus breeds a tight-knit community, and serving that community is contagious."
"To me, Gustavus provided a community like no other," he says. "I was surrounded by inspiring professors, coaches, and peers. Gustavus breeds a tight-knit community and serving that community is contagious. Professors inspired the pursuit of education and knowledge. Coaches encouraged setting goals and striving to achieve them." During his time at Gustavus, T.J. also participated in the Tau Psi Omega fraternity, the Student Athlete Volunteer Educators (SAVE), and worked as a biology teaching assistant.
Those years of athletic competition and academic focus certainly helped prepare him for the night he got a call from the pediatric emergency department. "It was this past winter and I was on call during a blizzard. They needed help with a seven-year-old girl who had a severely broken and deformed arm," he says. "With more instinct than anything, I got my boots on, spent a good hour shoveling my car out and driving to the emergency room. I don't remember seeing another car or even plow on the road. My family couldn't believe I went in. It was then that I realized that I didn't even consider the risk that I had put myself in that night. It's moments like this that I realize I've found my true passion."
Through his personal, academic, and professional experiences, T.J. has learned that he's most satisfied when working to make the people around him better. "I was drawn specifically to orthopedic medicine because it offers the opportunity to not just increase patients' quantity of life, but their quality of life," he says. "I'm driven to restore patients back to the activities they love. I'm blessed that everyday I go into the hospital or clinic I feel I'm living my life of purpose."
Dr. T.J. Ridley - 1Dr. T.J. Ridley - 2Dr. T.J. Ridley - 3Dr. T.J. Ridley - 4Dr. T.J. Ridley - 5Dr. T.J. Ridley - 6Dr. T.J. Ridley - 7
Haley Coller '16
Eric Butorac '03
Charlie Conn '94
Ferial Mohamed Pearson '01
Matt Rasmussen '98
Carly Zucker '07
Kate Schulze '15
Elin Ahldén '99
Brian J. Evans '07
Lieutenant Wes Jones '11
Dr. T.J. Ridley '10
Elizabeth (Truong) Jenson '05
Dr. Bernard Powers '72
David "Agape" Scherer '99
Ellen Ruiters '97


Japan is very famous of its maple leaf during the autumn. Other than the food, it is also one of the reason so many tourists visiting Japan every autumn.
Instead of featuring those popular tourists spot of maple leaf, this time we want to bring you to a not-so-crowded maple leaf spot. It is call Momiji Road (Maple Leaf Road in Japanese), located in south of Chiba Prefecture.
Since this location can only be accessed by car, not bus & train service. Local likes to drive along this country road to enjoy the view of Momiji during Autumn. It is a very long road, but it is very easy to know which area is the famous photography spots, as you can notice that by seeing cars parked at the road side.
Remember to keep yourself warm while enjoying the maple leaf on Momiji Road.


Alignment nanofibers of PAni.CSA/PEO blends with different concentration of polyethylene oxide (PEO) have been prepared using the electrospinning technique. The details of the preparation method are well described. The method is relatively simple and is easily controlled. A systematic investigation on the effect of annealing temperature on the structure of PAni.CSA/PEO nanofibers was studied. Morphology and diameters of the as-spun and annealing nanofibers were studied byAtomic ForceMicroscope and found the annealing increases the nanofiber diameter and had clear effect on the morphology and orientation of nanofibers. The X-ray diffraction analysis shows the effect of annealing on the nanofibers PAni.CSA/PEO crystallization is unsystematic and depended on the concentration of PEO in the blend.


The Clover Practice™ is described in the book Staying Healthy in Sick Organizations: The Clover Practice™. This practice is a means for achieving less stress and more peace of mind in the workplace. Three principles make up The Clover Practice™: tell the truth; always speak for yourself; and declare your interdependence (read carefully; not independence). The author claims workplaces tend to be fundamentally unhealthy because of obsolete organizing principles of hierarchy and patriarchy and command and control systems, the fact that too many managers and supervisors are not prepared to manage or supervise others, and the willingness to maintain organizational illusions.A practice is something you do every day regardless of the circumstances.
If peace of mind and reduced stress is our intention, we have to tell the truth even when it's uncomfortable, or inconvenient or we don't look good. White lies and unethically cutting corners compromise our integrity and the degree to which others trust us. This doesn't mean we "tell our truth" to everyone who comes along. But it does mean that "my truth" is just that. It's my opinion, not universal Truth.
Speaking to others about how things look from your perspective, history, memory and experience is a more productive and healthier way to be heard than telling people they are careless, uncooperative, lazy, incompetent, and unprofessional, etc. If you're clear you're speaking from your own observations and are open to and are able and willing to hear others' views, you are more apt to be heard.
No one succeeds alone – no one – even if they think they do. If you truly believed you need others in your organization – regardless of title, position, salary, etc. – to succeed, what would you do differently? You might be more inclined to interact and communicate with, and be openly grateful for, others up and down your organization.
Organizations are living organisms. It's often a challenge to consciously view, or understand, how what you do (say, feel…) affects others – on many levels. When you understand these connections (and consequences) more clearly, you might choose to "do" and "be" differently – which produces greater harmony and collaboration than dis-harmony, competition and conflict.
As a leader, manager, supervisor or employee, do you create a space or container where others feel safe and secure when speaking openly and honestly to/with you? Do you listen and hear? Do you seek clarification and understanding by probing and always digging deeper for clarity? Do you focus on the information, not the personality?
Speaking for yourself means you discuss your experience – the who, what, where, when, why and how. You stay away from using "you," "we," "them," "they," "everyone" and the like. Literally, you speak for your self. And no one else. Your perspective. Your observation. Without judgment. Without criticism.
Where, when and how do your see yourself as part of a larger whole? As a cell in the larger body of your organization? With whom do you interact – directly or indirectly – inside and outside the physical (or digital) walls of your organization? How do you support others and how do they support you to create results, reach goals, problem solve, resolve conflict and achieve?
You might work in a "smart" organization. However, this practice can and will support you and your colleagues – from the mail room to the 52nd floor – create a culture of safety and security, honesty and integrity, and inclusion and respect – all qualities of a "healthy" organization.
Of the three clovers, which is the easiest for you? Which is the most challenging? How so?
When are you most comfortable telling the truth? Least comfortable? How so?
How are you when it comes to speaking for yourself? Do you tend to use "we," "everyone" and the like (rather than "I")?
Do you experience interconnectedness at work (or elsewhere in your world)? How so?
What is your comfort level when working with/on a team? How so?
On the way, they set aside their dreams (once, real dreams) and tailor their lives and personalities to what the market demands. They practice the arts of "power dressing," power lunching, having or creating "winning personalities," all the while steeped in a state of emptiness, leading to unhappiness and dissatisfaction. In order to be "somebody," they burn out without ever having been on fire.
What is it about work that leads so many to be dissatisfied?
A special issue of Time Magazine (1/17/2005) featured an article about what is known as "reference anxiety"  "keeping up with the Joneses"  constantly comparing one's self and one's "stuff" with someone else's. Much of this takes place in (but is not restricted to) work environments and is characteristic of many of today's workplace cultures.
Perhaps the dissatisfaction element lies on a much deeper level of the psyche: it's about the inner person, not about the externals.
In other words, it's not the work that's at cause when it comes to worker dissatisfaction.
It's curious that of the thousands of business books that are published each year, there's hardly one chapter devoted to friendship in the workplace (real and true friendship, not the "good-old-boys, back-slapping stuff," that is a faux substitute. (And a bit of information: did you know that when two folks come together and pat each other on the back, it's because they cannot connect emotionally? When two folks honestly and sincerely connect, from their deeper self, from their heart, from a place of true love and connection, they hug and hold one another…they don't pat one another's back. Patting is a "faux" form of connection.).
Relationships rule the world, even the world of work. Finding meaning rules one's deeper sense of happiness, fulfillment, and well-being, even in the world of work. It's relationships, first with yourself, then with others, that must be examined to explore the true and real root causes of employee dissatisfaction.
The spirit of an organization begins and ends with the spirit of each individual. When we come to life with the right values, we are grounded on a foundation of truth, honesty, sincerity, and self-responsibility, and from this place, dissatisfaction can more easily morph into satisfaction.
So, really, really, why is worker satisfaction falling?
Am I constantly comparing myself to others and feeling I'm coming up short? How so?
Do I feel like a victim of life/work much of the time? Why?
Do I have true and real friendships at work?
Could I be contributing to my own dissatisfaction at work? If so, how? Honestly.
Do I have an expectation that my company or manager is responsible for my happiness at work?
What is it about work that excites me? If nothing or, "not much," then why do I choose to remain there? How might I proactively turn this around?
What personal and professional goals have I set for myself at work If I don't have any, could that contribute to my unhappiness?
Do I find meaning in my work? If not, why not?
Do I shop incessantly, max out my credit cards on stuff, and still feel empty and unhappy? Why?
What lessons did I learn about myself at work last year? I did learn some lessons, didn't I? How can I leverage these lessons to increase my satisfaction at work this year?
What mutually-supportive relationships and true friendships do I want to cultivate at work?
What self-defeating habits do I want to eliminate?
Are there toxic people in my life at work (or at home) who contribute to my unhappiness?
Who can I serve, support, coach or mentor that will bring me satisfaction or increase my happiness at work?
How have I grown at work during the past year? I have grown in some positive way, haven't I? If not, why not?
What one or two baby steps can I take this week or this month that can increase my satisfaction at work?
What did I learn about satisfaction and the world of work when I was growing up? How so?
So You Think You Can…Lead?
Not too long ago I was watching the TV show, "So you think you can dance," a show where contestants vie to become the winner in what is a weekly "dance-off" competition. The contestants dance solo and in pairs depending on the night's agenda. They're very good.
So, on that night, one of the judges was discussing one contestant's relationship to his partner in a hip-hop routine where an "emotional, contentious dynamic" between the pair was built into the storyline of their dance.
When the couple completed their routine, the male of the pair maintained a scowl, a macho "I-have-control-over-you!" non-verbal persona as he and his partner walked forward to center stage to receive the judges' feedback. As he approached, his scowl melted. He and his partner embraced and one could feel the energy of their connecting.
Hmmm, I thought, can't that same description apply to what makes for a successful, even sensational leader?
In today's face-paced, challenging, often-ambiguous and uncertain economic climate, where stress is rampant and anxiety and fear seem to be the emotions of choice driving many leaders' behaviors, more and more leaders seem to be losing touch with their employees, fostering a climate where poor morale, dis-engagement, absenteeism, presenteeism, stress, overt or silent anger and resentment abound. Why? Many leaders (and managers!) are severing their emotional ties to their workforce, assuming they had any emotional ties to begin with. They're leading their employees and if they are "dancing" with their employees, it's all technical and tactical there's no emotional connection.
Competencies, skills, talent, intellect, technical knowledge, expertise and drive define many of today's leaders. But, that's not enough.
What's happening in the face of challenging times is a rush to put into place the technically efficient leader, the "numbers guy," the "turnaround artist," the "visionary," etc., and in the process many organizations are experiencing the fallout from leaders who are technically savvy but who are clueless when it comes to "people" skills, who lack the emotional maturity and competence to truly lead.
The downside of the emotional disconnection is: unconsciously or consciously, they tend to push their "partner" away -generating internal conflict and competition when there could (should?) be compromise, collaboration and cooperation. They reject and repel their colleagues, their peers, their direct reports, even those who are as, or more, skilled and whose partnership they need in order to succeed.
With a focus on the technical – e.g., the bottom line, the strategic plan and the like – they effort and struggle, lacking greater self-awareness and emotional maturity. Eventually, when they come center stage for feedback, they are asked to leave the stage. They thought they could lead; technically they could, but it wasn't enough.
Take the time to learn to lead "people." Technical skills are not enough. Use the support of a qualified coach or mentor who can support you to understand the tasks AND the personal aspects of workplace relationships.
Learn to take risks, and experience failure as an opportunity through which self-reflection becomes a stepping stone to emotional learning and self-development.
Consciously and self-responsibly explore any tenuous relationships you have with others and search for root-cause issues that foster such relationships. Ask for a qualified coach to support you in your exploration.
Check your ego at the door and work to eliminate behaviors that are characterized as arrogant, bullying, aloof, or emotionally or verbally abusive. Again, seek the support of a coach or trusted friend or colleague who can help you in this endeavor.
Learn how to connect emotionally, authentically, as a human being, not just "officially" in a business context. To be professional and effective in these changing times requires a "greater humanity" – that is the capacity to conduct business with an open, compassionate and intelligent heart.
When it comes to "dancing" at work, do you always feel the need to lead? What would it be like to follow?
Do you always need to be center stage, in the limelight? If so, why?
Would you describe yourself as emotionally mature? How do you know? What would your colleagues, friends, or family say? Would you ask them?
Do you tend to be "officious," "all-business" or aloof in your relationships at work? What about at home or with others?
Do you have a need to be "right?" Would you generally prefer to be right than be happy? Do you ever gang up on or bully others? If so, why?
Would you consider yourself "well-rounded?" Would others agree with you?
Do you consider your boss(es) to be emotionally mature? Why, or why not?
Did you learn about emotional maturity as you were growing up? How so? Was it a pleasant or painful experience?
Can you envision a world where emotional maturity is a common attribute for most people?


On September 27, ActionAid, UN Women nk Sweden Local Association Uppsala and Female Integrity RISK Uppsala arrange a seminar to pay attention to and discuss methods to stop female genital mutilation in Sweden.
During the seminar, three invited language pipes from Somaliland will share their experiences from the work on female genital mutilation in Somaliland.
Help us acknowledg the International Day of Zero Tolerance for Female Genital Mutilation by joining out one-day seminar on the topic of ending FGM.
On Saturday the annual Culture night is hold in Uppsala and the organization SIU celebrates 30 years by inviting everyone to a day full of interesting events.
Female Integrity arranges a traditional Ethiopian coffee ceremony at 15:25.
END FGM European Network, which Female Integrity is a member of, are seeking artists/photographers for a photo exhibition on the theme "Building bridges to end female genital mutilation".
Today was the first meeting of the Swedish Change Agents. Change is an EU project aiming to spread knowledge and work for an abolishment of FGM through "Change Agents".
Today is the International Day of the Girl Child.
Read more at AWEPA's website.
TERRE DES FEMMES is launching an international project on Female Genital Mutilation within African communities in the European Union.
Read the invitation (PDF document).
Our sister organisation RISK is writing about recent news about FGM around the world.
On may 21 a round table discussion was held on the topic: Building Bridges between Europe and Africa, here is a short summery of the discussion.
On the occasion of International Day of Elimination of Violence against Women, Amnesty International's END FGM European Campaign has launched a Europe-wide action to raise at least 8,000 signatures on rose petals in solidarity with the 8,000 girls and women worldwide who are forcibly subjected to the practice of female genital mutilation (FGM) every day.
Sign the form or read more about the campaign.
This campaign digest, released on the occasion of Mother's Day, addresses the need to address FGM as an underlying cause of the lack of progress on the Millennium Development Goals. In particular, FGM and its ill-effects prevent achievement of MDG 3, 4, 5 and 6.
In advance of International Day of Zero Tolerance to female genital mutilation (FGM) on 6 February, Amnesty International's END FGM European Campaign calls on European leaders to support its strategy to protect young girls and women affected by FGM.
END FGM is a campaign run by Amnesty International Ireland, in partnership with non-governmental organisations across the European Union and Female Integrity is one of these NGOs.


Book your Lisbon transport out of the airport in advance and avoid the hassle, confusion and potential drama of splitting up and finding enough cabs.
Our guide will get you all on board your own coach and the driver will already know where you're going. So all you have to concentrate on is getting the party started!
Lisbon Transport – limo style!
You get off the plane, get your bags, walk out into the bright white airport lights and there someone in a smart uniform holding a sign with your name on it!
Yep, it's limo time. Your personal chauffeur will lead you to your luxury Lisbon transport vehicle, where you can just sit back and crack open the champers.
It really is a nice feeling pulling up to your accommodation, having your door opened for you and stepping out of this seriously cool car.
The only problem is that you could definitely get used to it!
Your flights are booking, accommodation sorted, activities chosen. Now how do we get to where all the action is? We can, of course, help with that with out Lisbon transport.
Airport's can be confusing, especially when you are trying to shepard about a group of lads, who have possibly started the party early, or the rest of the girls who cracked open the champagne on the flight. Our airport Lisbon transport service is an easy, hassle free solution.
We have affordable, comfortable coaches that will mean your group can stay together and arrive into the fantastic city of Lisbon together. Or if you're feeling in need of a little rock star treatment, then a Lisbon transport limousine door to door service, perhaps with a scenic tour along route, may be just the thing.
Lisbon itself is full of beautiful cobbled streets and hip hidden quarters, which can be confusing, so let out experienced local driver's take you to exactly where you're going. Avoid that awkward moment in front of your friends when you try to pronounce where you're staying to a cab driver who just looks at you like you're insane.
Once you are in Lisbon, it's a great city to walk around. There's also a really good tram service, that you can hop on and of, whenever you see a bar or restaurant that you fancy trying out. Or how about a segway tour? That way you can avoid those, challenging after several drinks, hills that Lisbon has. And of course a trip down the river is a must. You could even combine the 2 with a land and sea tour.
Meet & Greet no bleat!
Has to be the ride of a lifetime!


Macadamia nuts are nuts from Hawaii and are amazing to put in different healthy salad recipes. When you're looking for healthy salads to eat, include healthy fats along with several vegetables and greens. Use vegetables, fruits, and nuts that mimic the colors of the rainbow to get the best nutritional content. A good way to make different healthy salad recipes filling is to include nuts, such as macadamia nuts, and avocados.
Slice radishes, cucumber, carrots, and cabbage.
Dice avocado. Remove cilantro leaves from stems.
Nature's Eats Macadamia Nuts so that your salad looks as beautiful as a rainbow.
Keep the dressing simple either by using the one recommended above or a simple balsamic vinaigrette.
The variety of vegetables included in this salad will make each and every bite very exciting. You'll be extremely satisfied with the macadamia nuts along with avocados as these two ingredients add in creaminess and leave you feeling grounded. The slight sweetness from the dressing with the tangy vinegar and lemons bring lots of flavor to the neutral vegetables included in this amazing salad.


100 Students Involved In Black-on-Hispanic Brawls At NY School... is one of the headlines on the Drudge Report right now, right between Dead goldfish offered the vote in Illinois... and 76-Year-Old NYC Pickpocketer Arrested For 73rd Time!
But that's Drudge's headline—the actual WCBSTV headline is Hempstead High On Guard Following 2 Days Of Brawls Principal: 100 of School's 1,600 Students Involved; Dozens Suspended And Undercover Cops Take Over Building , Oct 21, 2008.
Hempstead is one of the few Black and Latino majority neighborhoods on Long Island (along with Roosevelt, Uniondale, Freeport and Wyandanch). It is also home to a large Salvadoran population.
But besides the "Uh-oh" there's the media point—the "black vs. Hispanic" thing belongs in the headline, where Drudge, with his ever reliable tabloid instincts, put it. And the media needs to know that, because there'll be more of these riots.


A Skeleton of Desire was published by Garron Publishing in October 2018 as part of their Southern-Land Poets Chapbook series.
It contains 10 poems that are mostly based on the human body in various ways – the organisation of the bones in the arms, their muscles, their development, dysfunction and recovery. Much of the imagery is derived from re-interpreting the original meanings of the latin names for body parts, diseases, and the environment they exist within.
Most of these poems have been previously published, with the five cardinal signs of inflammation and High Dependency originally appearing in the Medical Journal of Australia. Sensurious (Works on Paper) is derived from texts accompanying an exhibition of drawings by Judy Morris that were then used to create a video which was shortlisted for the Red Room Company / Royal Botanic Gardens New Shoots Poetry Prize, 2016. Dial Tone was awarded third place in the University of Canberra Health Poetry Prize 2017. No Glutamate is based on a scientific paper published with Judy Morris and our colleagues about the underlying neural pathways mediating pain.
If you'd like a copy, click here to place an order.