text:
\section{Introduction}
\end{center}

Thanks to the study of electro-magnetic duality initiated by Seiberg and
Witten, \cite{SW} the prepotential of the low energy effective action of
$N=2$ supersymmetric Yang-Mills theory was turned out to be viewed as a
function on a complex projective space having singularities when
the masses of charged particles vanish. This complex projective
space can be identified with the moduli space of a Riemann surface
determined by several physical requirements, thus the effective
theory can be considered to be controlled by the geometry of moduli space
of a Riemann
surface. \cite{KLYT,AF,HO,MN,DS1,DS2,Han,BL,APS,AAM,LPG,AAG,MW,LW,EY}
According to this observation,
since the effective coupling constants of the theory is interpreted as
the period matrix of a Riemann surface, determining the period matrix from
calculation of periods becomes equivalent to
evaluate effective coupling constants. It is interesting
that the instanton contributions to prepotential \cite{Sei}
can be obtained from the evaluation of periods and the prepotentials
obtained in this way \cite{KLT,IY,O,Matone,EFT,EF,Ito,Ghe,IS}
are known to be consistent to the instanton
calculus. \cite{IS,FP,IS3,Slat,DKM,HS,AHSW,Y}
In these studies, the method based on Picard-Fuchs equations
\cite{KLT,IY,O,Matone,EFT,EF,Ito,Ghe,Ryang,GSA,IMNS,Ali,O3} played a
crucial role.

However, on the one hand, the theory of prepotential often shows
unexpected aspects behind the effective theory. For example,
it is known that the Seiberg-Witten solutions can be understood in the
framework of Whitham theory. \cite{GKMMM,NT} Gorsky {\em et al.} \cite{GMMM}
noticed that the Whitham dynamics in $N=2$ Yang-Mills theory could
be written essentially by only finite number of Whitham times and
found that the second-order derivatives of prepotential over the
Whitham times could be represented by an elliptic function associated with
Seiberg-Witten curve.

However, we can further learn more aspects of Whitham hierarchy
in gauge theory from the basic idea of Gorsky {\em et al.}. \cite{GMMM}
For instance, note that since the number of time variables of the hierarchy
is restricted to be finite the generating meromorphic
1-form of the Whitham hierarchy is represented by a finite linear
combination of meromorphic 1-forms associated with these Whitham times.
Then we can expect that there must be closed differential relations among
these meromorphic differentials associated with Whitham times.
In fact, a detailed study supports this
observation and the aim of the paper is to show the consequence of
these relations, especially, a connection to Picard-Fuchs equations
for the Seiberg-Witten periods.

The paper is organized as follows. In Sec. II, we briefly summarize the
Whitham dynamics in SU($r+1$) gauge theory. In addition, following to
Gorsky {\em et al.}, \cite{GMMM} we consider the
situation that the number of Whitham times is finite.
Since the meromorphic 1-forms on Seiberg-Witten curve consisting of the
Whitham hierarchy must be always represented by simply a linear combination
of Abelian differentials, we can expect the existence of differential
relations among these meromorphic 1-forms. In Sec. III, it is shown that
such relations can be in fact found and as a result
Picard-Fuchs equations for the Seiberg-Witten periods are available
from this view point. It should be noted
that the generating meromorphic differential of the Whitham hierarchy can
be written in terms of the Seiberg-Witten 1-form. This indicates that
it is sufficient to consider only the Seiberg-Witten periods in order to
calculate the periods of the Whitham hierarchy. In Sec. IV, it is
shown that the SU(3) Picard-Fuchs equations for the Seiberg-Witten periods
can be obtained from the Picard-Fuchs equations with Whitham times
for the periods of the Whitham hierarchy by considering the specialization
condition to Seiberg-Witten model. Sec. V is a brief summary.

\begin{center}
\section{Whitham hierarchy in gauge theory}
\end{center}

In this section, we briefly sketch the relation between Seiberg-Witten
solution and Whitham dynamics in the context of
$N=2$ supersymmetric Yang-Mills theory. \cite{GKMMM,NT,GMMM}

\begin{center}
\subsection{Seiberg-Witten solution}
\end{center}

To begin with, let us recall that the Seiberg-Witten curve in SU($r+1$)
gauge theory without matter hypermultiplets \cite{KLYT,AF,HO}
is given by the characteristic equation
	\beq
	\det [x-L(\omega )]=0
	\lab{lax}
	\end{equation}
of the Lax operator $L(\omega )$ for Toda chain with $r+1$
sites, \cite{GKMMM} where $x$ is the eigenvalue of $L(\omega )$ and
$\omega$ is the spectral parameter. (\ref{lax}) can be rewritten in the
form of spectral curve
	\beq
	P(x)=\Lambda_{\mbox{\scriptsize SU($r+1$)}}^{r+1}
	\left( \omega +\frac{1}{\omega}\right)
	\lab{Luke-Skywalker}
	,\end{equation}
where $\Lambda_{\mbox{\scriptsize SU($r+1$)}}$ is the dynamical mass parameter
and
	\beq
	P(x):=x^{r+1} -\sum_{i=2}^{r+1}u_i x^{r+1-i}
	\end{equation}
represents the simple singularity of type $A_r$ with moduli $u_i$. This
spectral curve (\ref{Luke-Skywalker}) can be further rewritten in the
familiar hyperelliptic form \cite{KLYT,AF,HO}
	\beq
	y^2 =P^2 -4\Lambda^2
	,\lab{SWc}
	\end{equation}
where $\Lambda :=\Lambda_{\mbox{\scriptsize SU($r+1$)}}^{r+1}$ and we have
introduced
	\beq
	y :=\Lambda_{\mbox{\scriptsize SU($r+1$)}}^{r+1}
	\left( \omega -\frac{1}{\omega}\right)
	.\end{equation}
Note that the hyperelliptic curve (\ref{SWc}) is a Riemann surface of
genus $r$.

For a study of Riemann surface, it is often useful to consider
the periods of Abelian differentials over the 1-cycles on the surface.
In the case at hand, we can take $2r$ 1-cycles
$(A_i ,B_i )$ $(i=1,\cdots,r)$ on (\ref{SWc}) as a canonical basis ($B_i$
are symplectic duals of $A_i$), which can be expressed by using the
branching points of (\ref{SWc}).

On the other hand, in order to interpret the components of period
matrix constructed from periods of Abelian differentials as the
effective coupling constants, the combination of Abelian differentials must
be fixed uniquely up to total derivatives. In addition, in general, there
are three kinds of Abelian differentials on a Riemann surface, but that of
the third kind is not required here because we are considering a pure gauge
theory. Therefore, the expected meromorphic differential 1-form is
expressed by the Abelian differentials of the first and second kinds, and
the one satisfying these requirements is called Seiberg-Witten
differential $dS_{\mbox{\scriptsize SW}}$, given by
	\beq
	dS_{\mbox{\scriptsize SW}} :=x\frac{d\omega}{\omega}
	=x\frac{\partial_x P}{y}dx
	\lab{26}
	,\end{equation}
where we have ignored the numerical normalization for simplicity,
and then the Seiberg-Witten periods are given by the
loop integrals over the canonical cycles
	\beq
	a_i :=\oint_{A_i}dS_{\mbox{\scriptsize SW}}
	,\ a_{D_i}:=
	\oint_{B_i}dS_{\mbox{\scriptsize SW}}
	.\end{equation}
Note that $dS_{\mbox{\scriptsize SW}}$ can be viewed as the canonical 1-form
of the integrable system. In this way, we can see the relation between
Seiberg-Witten solution and integrable system.

\begin{center}
\subsection{Whitham hierarchy}
\end{center}

We have seen that the Seiberg-Witten solution has a connection to integrable
system, but it can be also viewed as a part of Whitham theory of solitons
on a Riemann surface.

To see this, let us recall that in general Whitham theory consists of the
following three ingredients: \cite{Kri}
	\begin{itemize}
	\item
	Riemann surface of genus $g$.
	\item
	Punctures on the surface.
	\item
	Existence of local coordinates near the punctures.
	\end{itemize}

Gorsky {\em et al.} \cite{GMMM} noticed that the meromorphic differentials
of the second kind $d\Omega_n$ of $(n+1)$-th order punctures $(n>0)$ on a
Riemann
surface was defined up to a linear combination of $g$ holomorphic
differentials $d\omega_i$ and considered how to fix this combination by
taking two basic requirements. The first one was to require
	\beq
	\oint_{A_i}d\Omega_n =0
	\end{equation}
and the second one was to introduce new meromorphic differentials $d\widehat{\Omega}_n$
which enjoy the property that their differentiations over the moduli
coincide with holomorphic differentials.

According to their result, \cite{GMMM} the differential
	\beq
	dS :=\sum_{n=1}^{\infty}T_n d\widehat{\Omega}_n =\sum_{i=1}^{g}\alpha_i
	d\omega_i +\sum_{n=1}^{\infty}T_n d\Omega_n
	\lab{29}
	\end{equation}
with infinitely many parameters $T_n$ called Whitham times is found to be
the expected solution which is suitable for applications to gauge theory.
For this new meromorphic differential $dS$, the
periods
	\beq
	\alpha_i :=\oint_{A_i}dS ,\ \alpha_{D_i}:=\oint_{B_i} dS
	\lab{211}
	\end{equation}
can be defined in a natural way.

Next, in order to make a contact with Seiberg-Witten solution,
Gorsky {\em et al.} \cite{GMMM} regarded the Riemann surface used here as
the Seiberg-Witten hyperelliptic curve (\ref{SWc}).

In such a situation, they found that the Whitham hierarchy could be
actually written by only first $r$ time variables and gave an explicit
expression of $dS$. In particular, in the case of SU($r+1$) gauge theory,
$n$ is restricted to $n<r+1$. Namely, in this situation, the periods
(\ref{211}) reduce to
	\beq
	\alpha_i =\sum_{n=1}^{r}T_n \oint_{A_i}d\widehat{\Omega}_n
	,\ \alpha_{D_i} =\sum_{n=1}^{r}T_n \oint_{B_i}d\widehat{\Omega}_n
	\lab{Yoda}
	\end{equation}
and $d\widehat{\Omega}_n$ are given by
	\beq
	d\widehat{\Omega}_n =R_n \frac{d\omega}{\omega},\ R_n :=P_{+}^{n/(r+1)}
	.\lab{33}
	\end{equation}
In this expression, $P_{+}^{n/(r+1)}$ means the non-negative terms
in the expansion of $P^{n/(r+1)}$ for a large $x$, and in general,
$P^{n/(r+1)}$ in SU($r+1$) gauge theory is easily found to give
	\beq
	P^{n/(r+1)}  =x^n -\frac{n}{r+1}u_2 x^{n-2}-\frac{n}{r+1}u_3 x^{n-3}-
	\frac{n}{r+1}\left[u_4 +\frac{u_{2}^2}{2}\left(1-\frac{n}{r+1}
	\right)\right]x^{n-4}-\cdots
	.\end{equation}

Note that the periods are now represented by a finite linear
combination of $d\widehat{\Omega}_n$ because we are considering only for $n<r+1$ case.
In addition, from (\ref{33}), it is immediate to see that the
Seiberg-Witten solution is recovered at the point
	\beq
	(T_1 ,T_2 , T_3 , \cdots ,T_r )=
	(1,0,0,\cdots ,0)
	\lab{Mr.Spok}
	.\end{equation}
In fact, we find $d\widehat{\Omega}_1 =dS_{\mbox{\scriptsize SW}}$. Of course,
in this case, we have $dS=dS_{\mbox{\scriptsize SW}}$.

\begin{center}
\section{Picard-Fuchs structure behind Whitham hierarchy}
\end{center}

\begin{center}
\subsection{Relations among meromorphic differentials}
\end{center}

We have seen that $dS$ is represented by a linear combination
of $d\widehat{\Omega}_n$ and also seen that $d\widehat{\Omega}_1 =dS_{\mbox{\scriptsize SW}}$.
Then, are $d\widehat{\Omega}_n$ for $n \neq 1$ related to
$dS_{\mbox{\scriptsize SW}}$? If we can find any relation among them,
the role of the Seiberg-Witten solution in the Whitham dynamics will be
clarified.

To find an answer to this question, let us notice that any
meromorphic differential on a Riemann surface must be always
written in terms of the basis of Abelian differentials on the
surface. Of course, this must be true also for $d\widehat{\Omega}_n$ for
all $n$. Therefore, if we consider a differentiation of $d\widehat{\Omega}_n$
over moduli, it will be ultimately represented by a linear combination of
various $d\widehat{\Omega}_n$ and their derivatives.
However, actually, in the case of Seiberg-Witten Riemann surface,
we can show that the derivatives of
$d\widehat{\Omega}_n$ for $n>1$ are obtained from the Seiberg-Witten differential
$d\widehat{\Omega}_1$. Thus as the result, we can conclude that
$dS$ is generated from $d\widehat{\Omega}_1$ and accordingly the periods of $dS$ can be
directly determined through the Seiberg-Witten periods themselves.

To see this more concretely, let us consider the case of $d\widehat{\Omega}_2$ as an
example. Since the differentiations of $d\widehat{\Omega}_2$ over moduli are
	\beq
	\frac{\partial d\widehat{\Omega}_2}{\partial u_i}=\frac{dx}{y}
	\left[ -2\delta_{2,i}x^{r} +\frac{\delta_{2,i}}{r+1}\sum_{j=2}^{r+1}
	(r+1-j)u_j x^{r-j} +2x^{r+2-i}\right]
	,\lab{31}
	\end{equation}
where $\delta_{i,j}$ are the Kronecker's delta symbols, and those
for $d\widehat{\Omega}_1$ are
	\beq
	\frac{\partial d\widehat{\Omega}_1}{\partial u_i}=\frac{x^{r+1-i}}{y}dx
	,\lab{32}
	\end{equation}
it is easy to see that
	\beq
	\frac{\partial d\widehat{\Omega}_2}{\partial u_2}=\frac{2}{r+1}\sum_{i=2}^{r+1}(r+1-i)
	u_i \frac{\partial d\widehat{\Omega}_1}{\partial u_{i+1}},\
	\frac{\partial d\widehat{\Omega}_2}{\partial u_i}=2\frac{\partial d\widehat{\Omega}_1}{\partial u_{i-1}} \ \ \
	(i\neq 2)
	.\lab{C3PO}
	\end{equation}
Note that in the derivation of (\ref{31}) and (\ref{32}) we have used the
general formulae
	\beq
	\frac{\partial d\widehat{\Omega}_n}{\partial u_i}=\frac{dx}{y}\left[\partial_{u_i}R_n \cdot
	\partial_x P -\partial_x R_n \cdot \partial_{u_i}P\right]+
	d\left(\frac{R_n \partial_{u_i}P}{y}\right)
	.\end{equation}

In a similar way, we can obtain differential relations between
$d\widehat{\Omega}_n$ for $n>1$ and $d\widehat{\Omega}_1$, but we omit the derivations for them
and show only the result for $n=3$ and $4$ cases here.

For $d\widehat{\Omega}_3$:
	\begin{eqnarray}
	& &\frac{\partial d\widehat{\Omega}_3}{\partial u_2}=-\frac{3}{r+1}\left[
	u_2 \frac{\partial d\widehat{\Omega}_1}{\partial u_2} -\sum_{i=2}^{r+1}(r+1-i)u_i
	\frac{\partial d\widehat{\Omega}_1}{\partial u_i }\right],\nonumber\\
	& &\frac{\partial d\widehat{\Omega}_3}{\partial u_3}=-\frac{3}{r+1}\left[
	u_2 \frac{\partial d\widehat{\Omega}_1}{\partial u_3} -\sum_{i=2}^{r+1}(r+1-i)u_i
	\frac{\partial d\widehat{\Omega}_1}{\partial u_{i+1}}\right],\nonumber\\
	& &\frac{\partial d\widehat{\Omega}_3}{\partial u_i}=3\left[ \frac{\partial d\widehat{\Omega}_1}{\partial u_{i-2}}
	-\frac{u_2}{r+1}\frac{\partial d\widehat{\Omega}_1}{\partial u_i}\right] \ \ \
	(i\neq 2,3)
	.\lab{35}
	\end{eqnarray}

For $d\widehat{\Omega}_4$:
	\begin{eqnarray}
	\frac{\partial d\widehat{\Omega}_4}{\partial u_2}&=&-\frac{4}{r+1}\Biggl[
	u_3 \frac{\partial d\widehat{\Omega}_1}{\partial u_2}-
	\sum_{i=3}^{r+1}(r+1-i)u_i \frac{\partial d\widehat{\Omega}_1}{\partial u_{i-1}}
	-\frac{r-3}{r+1}u_2 \sum_{i=2}^{r+1}(r+1-i)u_i \frac{\partial d\widehat{\Omega}_1}
	{\partial u_{i+1}}\Biggr],\nonumber\\
	\frac{\partial d\widehat{\Omega}_4}{\partial u_3}&=&-\frac{4}{r+1}\left[ 2u_2 \frac{\partial d
	\widehat{\Omega}_1}{\partial u_2}+u_3 \frac{\partial d\widehat{\Omega}_1}{\partial u_3}-\sum_{i=2}^{r+1}
	(r+1-i)u_i \frac{\partial d\widehat{\Omega}_1}{\partial u_i}\right],\nonumber\\
	\frac{\partial d\widehat{\Omega}_4}{\partial u_4}&=&-\frac{4}{r+1}\left[ 2u_2 \frac{\partial d
	\widehat{\Omega}_1}{\partial u_3}+u_3 \frac{\partial d\widehat{\Omega}_1}{\partial u_4}-\sum_{i=2}^{r+1}
	(r+1-i)u_i \frac{\partial d\widehat{\Omega}_1}{\partial u_{i+1}}\right],\nonumber\\
	\frac{\partial d\widehat{\Omega}_4}{\partial u_i}&=&4\left[ \frac{\partial d
	\widehat{\Omega}_1}{\partial u_{i-3}}-\frac{2u_2}{r+1}\frac{\partial d\widehat{\Omega}_1}{\partial u_{i-1}}-
	\frac{u_3}{r+1}\frac{\partial d\widehat{\Omega}_1}{\partial u_i}\right] \ \ (i\neq 2,3,4 )
	\lab{36}
	.\end{eqnarray}

\begin{center}
\subsection{Picard-Fuchs equations from Whitham hierarchy}
\end{center}

If the derivatives of $d\widehat{\Omega}_n$ over moduli for $n>1$ are eliminated from
the relations (\ref{C3PO}), (\ref{35}) and (\ref{36}) by using
differentiations, the equations satisfied by $d\widehat{\Omega}_1$ will be obtained.
Furthermore, since $d\widehat{\Omega}_1 =dS_{\mbox{\scriptsize SW}}$,
we can identify such equations as Picard-Fuchs equations for
Seiberg-Witten periods.

To see this, it is enough to consider the cross derivatives of $d\widehat{\Omega}_n$.
For example, for $d\widehat{\Omega}_2$, from $[\partial_2 \partial_i -\partial_i \partial_2]d\widehat{\Omega}_2 =0$,
where $\partial_i :=\partial /\partial u_i$, we get
	\beq
	\left[ (r+1)\partial_2 \partial_{i-1} -(r+1-i)\partial_{i+1}-\sum_{j=2}^{r+1}
	(r+1-j) u_j \partial_i \partial_{j+1} \right]d\widehat{\Omega}_1 =0 \ \ (i\neq 2)
	\lab{R2D2}
	,\end{equation}
which are the Picard-Fuchs equations obtained by several
authors. \cite{IS,Ali} For other $d\widehat{\Omega}_n$, we can construct similar
equations and, in fact, we can obtain the ``hierarchy'' of Picard-Fuchs
equations as follows:
	\begin{eqnarray}
	& &\left[\, \sum_{i=2}^{r+1}(r+1-i)u_i (\partial_3 \partial_i -\partial_2
	\partial_{i+1})\right]d\widehat{\Omega}_1 =0,\nonumber\\
	& &\left[ (r+1-i)\partial_{i+1} -(r+1)\partial_3 \partial_{i-2}+
	\sum_{j=2}^{r+1}(r+1-j)u_j \partial_i \partial_{j+1}\right]d\widehat{\Omega}_1 =0\ \
	(i\neq 2,3),\nonumber\\
	& &\left[(r+1)\partial_2 \partial_{i-2}-(r+2-i)\partial_i -
	\sum_{j=2}^{r+1}(r+1-j)u_j \partial_i \partial_j \right]
	d\widehat{\Omega}_1 =0 \ \ (i\neq 2,3),\nonumber\\
	& &\Biggl[ 2(r+1)u_2 \partial_{2}^2 +(r-3)(r-2)u_2 \partial_4 +
	(r+1)\sum_{i=3}^{r+1}(r+1-i)u_i \partial_{i-1}\partial_3 \nonumber\\
	& &\qquad\quad +(r-3)u_2 \sum_{i=2}^{r+1}(r+1-i)u_i \partial_{i+1}\partial_3
	-(r+1)\sum_{i=2}^{r+1}(r+1-i)u_i \partial_i \partial_2 \Biggr]d\widehat{\Omega}_1 =0,\nonumber\\
	& &\Biggl[ 2(r+1)u_2 \partial_2 \partial_3 +(r-3)^2 u_2 \partial_5 +(r+1)
	\sum_{i=3}^{r+1}(r+1-i)u_i \partial_{i-1}\partial_4 \nonumber\\
	& &\qquad\quad -(r+1)\sum_{i=2}^{r+1}(r+1-i)u_i \partial_{i+1}\partial_2 +
	(r-3)u_2 \sum_{i=2}^{r+1}(r+1 -i)u_i \partial_{i+1}\partial_4
	\Biggr]d\widehat{\Omega}_1 =0,\nonumber\\
	& &\Biggl[ (r+1)^2 \partial_2 \partial_{i-3}-2(r+1)u_2 \partial_{i-1}\partial_2
	-(r+1)(r+3-i)\partial_{i-1}\nonumber\\
	& &\qquad\quad -(r-3)(r+1-i)u_2 \partial_{i+1}
	-(r+1)\sum_{j=3}^{r+1}(r+1-j)u_j \partial_i \partial_{j-1}\nonumber\\
	& &\qquad\quad
	-(r-3)u_2 \sum_{j=2}^{r+1}(r+1-j)u_j \partial_i \partial_{j+1}\Biggr]
	d\widehat{\Omega}_1 =0 \ \ (i\neq 2,3,4),\nonumber\\
	& &\left[ 2u_2 (\partial_2 \partial_4 -\partial_{3}^2 )-
	\sum_{i=2}^{r+1}(r+1-i)u_i (\partial_4 \partial_i -\partial_3 \partial_{i+1})\right]
	d\widehat{\Omega}_1 =0,\nonumber\\
	& &\Biggl[ 2u_2 (\partial_3 \partial_i -\partial_4 \partial_{i-1})+(r+1)
	\partial_4 \partial_{i-3}-(r+1-i)\partial_{i+1}\nonumber\\
	& &\qquad\quad -
	\sum_{j=2}^{r+1}(r+1-j)u_j \partial_i \partial_{j+1}
	\Biggr]d\widehat{\Omega}_1 =0 \ \ (i\neq 2,3,4),\nonumber\\
	& &\Biggl[ 2u_2 (\partial_i \partial_2 -\partial_3 \partial_{i-1})+(r+1)\partial_3 \partial_{i-3}
	-(r+2-i)\partial_i \nonumber\\
	& &\qquad\quad -\sum_{j=2}^{r+1}(r+1-j)u_j
	\partial_i \partial_j \Biggr]d\widehat{\Omega}_1 =0 \ \ (i\neq 2,3,4)
	.\lab{310}
	\end{eqnarray}

Note that the equations in (\ref{310}) are all second-order equations and
in some cases we can simplify them by using
$(\partial_i \partial_j -\partial_p \partial_q )d\widehat{\Omega}_1 =0$, where $i+j =p+q$. \cite{IS,Ali}

\begin{center}
\subsection{Picard-Fuchs equations as a complete system}
\end{center}

Of course, as a complete Picard-Fuchs system, it is not necessary to
consider all equations in (\ref{R2D2}) and (\ref{310}). In general, since
there are $r$ moduli parameters in the SU($r+1$) gauge theory, it is
sufficient to extract at least $r$ independent equations from them.

To see this, let us notice the equations in (\ref{R2D2}).
Since the number of the equations is $r-1$, one more equation is
necessary. However, we can not obtain the expected equation from (\ref{310})
because the equations presented there do not have the instanton corrections.
If the instanton correction terms are not included in any one of
Picard-Fuchs equations, the prepotential obtained from them will
not show the instanton corrections precisely. Therefore,
we require that the remaining one must include instanton terms.

Actually, such equation was recognized by Ito and Yang \cite{IYY}
as the scaling relation. There, the Picard-Fuchs system was
realized by two kinds of equations, one of which is Gauss-Manin system and
the other is the scaling relation. Since the Gauss-Manin system does not
involve instanton corrections, the situation looks like our's. Therefore,
also for our case, the scaling relation may be used as the
remaining Picard-Fuchs equation.

For this, let us consider the Eulerian operator
	\beq
	{\cal{E}}:=\sum_{i=2}^{r+1}iu_i \partial_i +(r+1)\Lambda \partial_{\Lambda}
	\lab{Eu}
	,\end{equation}
which acts as
	\beq
	{\cal{E}}d\widehat{\Omega}_n =nd\widehat{\Omega}_n
	\lab{Eu2}
	\end{equation}
for all $n>0$. (\ref{Eu2}) indicates that the degree of $d\widehat{\Omega}_n$ is $n$.
Realizing (\ref{Eu2}) as an equation only in terms of
moduli derivatives can be easily accomplished by considering the squaring
equation $({\cal{E}}-n)^2 d\widehat{\Omega}_n =0$. \cite{Ali,IYY}

In this way, we can associate $r$ independent Picard-Fuchs equations
for $d\widehat{\Omega}_1$.

\begin{center}
\section{Picard-Fuchs equations with Whitham times}
\end{center}

\begin{center}
\subsection{The SU(3) Picard-Fuchs equations}
\end{center}

Next, let us consider Picard-Fuchs equations for the periods
$(\alpha_i ,\alpha_{D_i})$ of Whitham hierarchy. In the case of $r=1$,
the resulting Picard-Fuchs equation takes the same form with the usual
one \cite{KLT} up to rescaling of $T_1$. For this reason, we do not discuss
this case, and instead, let us consider $r=2$ case in order to find a
non-trivial example of Picard-Fuchs equations with Whitham times.

In this case, the Picard-Fuchs equations with the Whitham times are
found to be in the form
	\beq
	\L_j (\alpha_i ,\alpha_{D_i}) =0
	,\end{equation}
where
	\begin{eqnarray}
	\L_1&=&
	\frac{54u^2 vT_1 T_2 -(108\Lambda^2 -4u^3 -27v^2 )(uT_{2}^2 -
	3T_{1}^2 )}{u(-3T_{1}^2 +4uT_{2}^2 )}\partial_{u}^2 \nonumber\\
	& &-\frac{
	3[ (-108\Lambda^2 +4u^3 +27v^2 )T_1 T_2 +8uv(uT_{2}^2 -3T_{1}^2 )]}{
	2(3T_{1}^2 -4uT_{2}^2 )}\partial_u \partial_v \nonumber\\
	& &+\frac{T_2 [8(108\Lambda^2 -4u^3 -27v^2 )(-3T_{1}^2 +uT_{2}^2 )
	T_2 -9uvT_1 (15T_{1}^2 +28uT_{2}^2 )]}{2u(3T_{1}^2 -4uT_{2}^2 )^2}
	\partial_u \nonumber\\
	& &+\frac{2(108\Lambda^2 -4u^3 -27v^2 )(3T_{1}^2 -uT_{2}^2 )T_1 T_2
	+3uv(9T_{1}^4 +27uT_{1}^2 T_{2}^2 -4u^2 T_{2}^4)}{
	u(3T_{1}^2 -4uT_{2}^2 )^2}\partial_v +1,\nonumber\\
	\L_2&=&\frac{-54u^2 vT_1 T_2 +(108\Lambda^2 -4u^3 -27v^2 )(uT_{2}^2 -
	3T_{1}^2 )}{3(3T_{1}^2 -4uT_{2}^2 )}\partial_{v}^2 \nonumber\\
	& &-\frac{3[8uv(uT_{2}^2-3T_{1}^2)+(-108\Lambda^2 +4u^3 +27v^2 )
	T_1 T_2 ]}{2(3T_{1}^2 -4uT_{2}^2 )}\partial_u \partial_v
	-\frac{45vT_1 T_2}{2(3T_{1}^2 -4uT_{2}^2 )}\partial_u \nonumber\\
	& &+\frac{3v(3T_{1}^2 +uT_{2}^2 )}{3T_{1}^2 -4uT_{2}^2}\partial_v +1
	.\lab{pff}
	\end{eqnarray}

Though the derivation of Picard-Fuchs equations for other higher $r$ is
straightforward, the result is turned out to be too lengthy and
complicated, so we do not consider these cases in this paper.

\begin{center}
\subsection{Specializations of SU(3) Picard-Fuchs equations}
\end{center}

It may be instructive to see specializations of (\ref{pff}).
With the help of (\ref{Mr.Spok}),
it is straightforward to make sure that the equations in (\ref{pff}) yield
the usual SU(3) Picard-Fuchs equations \cite{KLT} $L_j (a_i ,a_{D_i})=0$
for the Seiberg-Witten periods, which can be identified with
Appell's $F_4$ system \cite{Er,Tak,Kato,Kan}
	\begin{eqnarray}
	& &\L_1 \rightarrow L_1 :=(4u^3 +27v^2 -108\Lambda^2 )\partial_{u}^2
	+12u^2 v \partial_u \partial_v +3uv\partial_v +u,\nonumber\\
	& &\L_2 \rightarrow L_2 :=(4u^3 +27v^2 -108\Lambda^2 )\partial_{v}^2
	+36uv\partial_u \partial_v +9v\partial_v +3
	\lab{L}
	.\end{eqnarray}
Note that the consistency condition of (\ref{L}) leads to
$[u\partial_{v}^2 -3\partial_{u}^2] (a_i ,a_{D_i})=0$,
which coincides with (\ref{R2D2}) for $r=2$.

On the other hand, from (\ref{pff}) with $(T_1 ,T_2 )=(0,1)$,
we can also consider Picard-Fuchs equations
$\widehat{L}_j (\oint_{A_i}d\widehat{\Omega}_2 ,\oint_{B_i}d\widehat{\Omega}_2 )=0$ for the periods
of $d\widehat{\Omega}_2$, where
	\begin{eqnarray}
	\L_1 \rightarrow \widehat{L}_1 &:=&u(4u^3 +27v^2 -108\Lambda^2 )\partial_{u}^2
	+12u^3 v\partial_u \partial_v -
	(4u^3 +27v^2 -108\Lambda^2 )\partial_u -3u^2 v\partial_v +4u^2 , \nonumber\\
	\L_2 \rightarrow \widehat{L}_2 &:=&(4u^3 +27v^2 -108\Lambda^2 )\partial_{v}^2
	+36uv\partial_u \partial_v -9v\partial_v +12
	\lab{ren}
	.\end{eqnarray}
From (\ref{ren}), we can obtain a relation like that from (\ref{L}), but
the same equation is also available from (\ref{C3PO}), provided
$\partial d\widehat{\Omega}_1 /\partial u_i$ are eliminated from (\ref{C3PO}).

Finally, note that we have
	\beq
	\widehat{L}_j (\alpha_i ,\alpha_{D_i}) =T_1
	\widehat{L}_j\left(\oint_{A_i}d\widehat{\Omega}_1 ,\oint_{B_i}d\widehat{\Omega}_1 \right)
	,\ L_j (\alpha_i ,\alpha_{D_i}) =T_2
	L_j \left(\oint_{A_i}d\widehat{\Omega}_2 ,\oint_{B_i}d\widehat{\Omega}_2 \right)
	\end{equation}
from (\ref{29}), (\ref{L}) and (\ref{ren}).

\begin{center}
\section{Summary}
\end{center}

In this paper, we have discussed the SU($r+1$) gauge theory in the
standpoint of Whitham dynamics and realized $r-1$
Picard-Fuchs equations for Seiberg-Witten periods as consistency
equations among meromorphic differentials associated with Whitham times.
In addition, we have used the scaling relation as the remaining independent
equation in order to include the instanton corrections. Though the
generalization to other cases except SU($r+1$) group is straightforward,
the case of exceptional gauge groups would be interesting because there are
two types of Seiberg-Witten curves in these gauge
theories. \cite{DS2,AAM,LPG,AAG,MW,LW,EY} In particular,
it may be interesting to know how the differences of physics expected
from these two curves \cite{LPG,EY,Ito,Ghe} are reflected in the Whitham
theory and the Picard-Fuchs structure behind it.

Of course, our construction of Picard-Fuchs equations may provide
helpful informations not only for these cases but also
when we consider the relation among flat coordinates, \cite{IXY,IY2}
Witten-Dijkgraaf-Verlinde-Verlinde
equations \cite{Wit,DW,DVV,MMM1,MMM2,IYYY} and Whitham
hierarchy. \cite{GKMMM,NT,GMMM} We are now planning a discussion
respect to this point.

\begin{center}

redpajama_set_name: RedPajamaArXiv


text:
Journal of Torbat Heydariyeh University of Medical Sciences
Volume 2, Issue 1 (4-2014) jms 2014, 2(1): 41-47 | Back to browse issues page
moshki M, alinejad J, hosseini Z, kameli M. Evaluation of iodine sufficiency in school children of torbathaydareyeh cite, province 2013. jms. 2014; 2 (1) :41-47
URL: http://jms.thums.ac.ir/article-1-90-en.html
Evaluation of iodine sufficiency in school children of torbathaydareyeh cite, province 2013
Mehdi Moshki 1, Javad Alinejad, Zohreh Hosseini, Mohammad Kameli
1- University of Medical Sciences Torbat Heydarieh Gonabad
Background and aim: Iodine deficiency accounts for a group of diseases such as Endemic goiter, hypothyroidism, Kirtinism and congenital anomalies. This study was carried out to monitor the national program for preventing iodine deficiency in 8-10 year old students in 1392 in Torbat haydareyeh city. Materials and Methods: In this cross-sectional survey, 487 students of both sexes, aged from 8-10 years were selected from urban and rural areas through cluster sampling. Urine samples were obtained and urinary iodine measured based on cholorimetery and acid digestion related to guidelines of Department of Endocrinology and Metabolism. Findings: The urinary iodine excretion median in evaluated students was 21 micrograms per deciliter and this amount in 62% population was between 10-30 micrograms per deciliter. Urinary iodine median of rural and urban students was 22 and 20 micrograms per deciliter, respectively that there was significant difference between these groups. In addition the urinary iodine median levels in boys and girls were 20 and 21 micrograms per deciliter that there was no statistically significant difference. Urinary iodine median in different regions are not the same and there was no significant difference in different regions. Findings of this study show that the urinary iodine median in students is desirable and higher than the national average. Conclusions: In this study, the urinary iodine excretion median is 20 micrograms per deciliter which indicates the absence of iodine deficiency in Torbat. The important issue in this study is that despite increasing urinary iodine median among the students as iodine deficiency correction index, urinary iodine median in 20% of students is less than 10 micrograms per deciliter. Therefore it is necessary to educate families for using food sources containing iodine such as eating fish at least twice a week and using refined iodized salt to reduce undesirable amounts of urinary iodine median.
Keywords: students goiter, iodine deficiency disorders, urinary iodine
Received: 2014/07/24 | Accepted: 2014/11/12 | Published: 2015/03/8
Torbat Heydariyeh University of Medical Sciences
Iranian Research Information System
Health, Journal, chimes, Journal of Torbat Heydariyeh University of Medical Sciences,
© 2020 All Rights Reserved | Journal of Torbat Heydariyeh University of Medical Sciences

redpajama_set_name: RedPajamaCommonCrawl


text:
Q: How to reset simulators for specific Xcode version using fastlane? Within gitlab-ci.yml I have:

test:
  stage: test
  before_script:
    - killall "Simulator" || true
  script:
    //how can I select proper xcode here?
    - bundle exec fastlane snapshot reset_simulators --force
    - bundle exec fastlane test
  after_script:
    - killall "Simulator" || true
    - rm -rf ~/Library/Developer/Xcode/Archives || true
  artifacts:
    name: "Staff_${CI_PIPELINE_ID}"
    paths:
      - fastlane/output/coverage
  when: on_success
  tags:
    - iOS

Why do I need to do that?
Because reset_simulators --force resets simulators for different xcode version than I use;) How can I force it to select good xcode version?

A: If you want this for scan or run_tests
It now supports
reset_simulator

Enabling this option will automatically erase the simulator before running the application
SCAN_RESET_SIMULATOR

just call
xcversion(version: 11.0)
run_tests(
    reset_simulator: true
)

A: It looks like you have your own Fastfile which has your test lane. I would suggest that you reset the simulators in there. Then add the xcode_select call before the reset.
For example:
lane :test do
  xcode_select('/Applications/Xcode9.4.1.app')
  Snapshot::ResetSimulators.clear_everything!(nil, true) # what reset_simulators ends up calling
  # your other code
end

A: Have you tried the fastlane action "reset_simulator_contents"
This will reset all simulators running on the test machine.

redpajama_set_name: RedPajamaStackExchange


text:
DEARS
PART 935 - RESEARCH AND DEVELOPMENT CONTRACTING
Department of Energy Acquisition Regulation
Authority: 42 U.S.C. 7101 and 50 U.S.C. 2401
Source: 49 FR 12016, Mar. 28, 1984, unless otherwise noted.
935.010 Scientific and technical reports.
935.070 Research misconduct.
935.071 Contract clause.
Parent topic: SUBCHAPTER F - SPECIAL CATEGORIES OF CONTRACTING
(c) All research and development contracts which require reporting of research and development results conveyed in scientific and technical information (STI) shall include an instruction requiring the contractor to submit all STI, including reports and notices relating thereto, electronically to the U.S. Department of Energy (DOE), Office of Scientific and Technical Information (OSTI), using the DOE Energy Link System (E-link) at http://www.osti.gov/elink. The phrase "reports and notices relating thereto" does not include reports or notices concerning administrative matters such as contract cost or financial data and information. The DOE Order 241.1B Scientific and Technical Information Management, or its successor version, sets forth requirements for STI management.
(d) As prescribed in DOE Order 241.1B, the contracting officer shall ensure that the requirements of the attendant Contractor Requirements Document are included in applicable contracts.
(a) Applicability. The DOE research misconduct policy set forth at 10 CFR part 733 addresses research misconduct by individuals who propose, perform or review research of any kind for the Department of Energy pursuant to a contract. The regulation applies regardless of where the research or other activity is conducted or by whom.
(b) Definition. Research misconduct means fabrication, falsification, or plagiarism in proposing, performing, or reviewing research, or in reporting research results. Research misconduct does not include honest error or differences of opinion. A finding of research misconduct means a determination, based on a preponderance of the evidence, that research misconduct has occurred, including a conclusion that there has been a significant departure from accepted practices of the relevant research community and that it be knowingly, intentionally, or recklessly committed.
The contracting officer must insert the clause at 952.235-71, Research Misconduct, in contracts, including management and operating contracts, that involve research.
DEAR Parts
Regulations Dears Menu


text:
Paris - Sleeping With the Enemy (CD, 1992)
When I was still in high school - this would have been around 1993 - I used to go down to Eugene and visit my off-and-on girlfriend who lived down there (long story). She lived in a house with a few girls, but there were always random people hanging around. I got to know a couple of guys who were always over there, through various Boone's-drinking, bong-hitting, and music-listening. One of the guys' names was Paul, but everybody called him P-Dog.
One night we were playing this idiotic game that P-Dog liked to play where you took a bong hit, held the smoke in, took a pull from a 40 of OE, ate a cookie, and then blew the smoke out. Seriously: I had to be seventeen to think this was as awesome as I did. Anyway. P-Dog and his friend had great taste in hip hop, and on this night, they were rocking something I'd never heard before. I was extremely out of it, but this music was blowing my mind. I asked them what it was, and they flipped me the CD. Paris. Sleeping With the Enemy. Just then, his voice rattled out of the shit speakers: "P-Dog the Bush killa." Ah.
We listened to the CD on and off whenever I was down there, but I would always forget to buy it. Which was weird, because I loved it. In fact, I don't think I picked it up until a few years later. I can't be sure of that. But I know I had it when I was 19, because I was fucking immersed in it by that point. (I put "Coffee, Donuts & Death" on a mixtape that year for my girlfriend, for chrissake. She hated it, and rightfully so.) Maybe I bought it the year before? It doesn't matter. I bought it, listened to it, and wondered why in the hell it took me so damn long to buy this album. Because it is amazing.
It's frustrating that Sleeping With the Enemy has become more well-known for its cover and content controversy (more about that here) than it has for its music. This is Paris' crowning achievement, an album that, while well-received at the time and still highly regarded in some circles, never got the universal props it deserved. The way this thing flows together as a collection of songs is seamless, and the beats that Paris put together manage to be more diverse, more powerful, and even more catchy than the ones he crafted for his debut.
"Make Way for a Panther," "Sleeping With the Enemy," and "House Niggas Bleed Too" are the first three proper tracks on the album, and they're all insane. Turns out they're just the prelude to the murder fantasy that everyone whined about, "Bush Killa." It's a great song, and that's all that matters. That's all that should have mattered. Anyway, the album starts out in mega-fierce mode (good move), but Paris mixes shit up as it goes along. "Assata's Song" and "The Days of Old" are both mellow and thoughtful tracks, and he pulls them off with ease.
Still, this album is at its best when he comes with the hard shit. "Guerrillas in the Mist" is actually part two of "Break the Grip of Shame" from The Devil Made Me Do It (it uses the same beat, even), and it sounds even grittier than it did the first time around. "Conspiracy of Silence" features Son Doobie from Funkdoobiest (listed in the liner notes as "Sun Dubious") and L.P. (?) and is one of the more bouncy tracks that Paris made up to this point. He also throws in some shorter, interlude-y cuts, as well as some slower knowledge-droppers. Great sequencing, great composition. Great one to listen to on headphones.
Oh, and a fun fact: A young DJ Shadow did some of his first recorded work on this record.
Many years ago, a friend of mine who worked at a record store unearthed an original, sealed copy of this CD, still in its longbox. Needless to say, it remains untouched and is on a shelf in my front room.
"The Days of Old"
Posted by Wockenfuss at 12:53 AM
Labels: 90's hip hop/rap, CD
I was one of those people that you forced Paris on with numerous mixtape appearances and I'll have to say that it worked. While I don't listen to this a ton it certainly has a time and a place. My jams are "Sleeping With The Enemy," "Bush Killa," and "Coffee, Donuts, And Death," the latter which gave me endless enjoyment as a younger man. This is the only Paris album I own but it always seems to do the trick when I want to hate stuff. I should totally work out to it. Good idea. I found listening to Ice Cube while working out does wonders.
Liz Phair - Exile in Guyville (CD, 1993)
I Went to a Show: Henry Rollins at the Aladdin The...
Pedro the Lion - Achilles Heel (CD, 2004)
Peanuts & Corn - Factory Seconds (CD, 2001)
Stallion Alert at the Movies: Pavement - Slow Cent...
Pavement - Live Europaturnén MCMXCVII (2) (LP, 2009)
Pavement - Live Europaturnén MCMXCVII (LP, 2008)
Pavement - Terror Twilight (CD, 1999)
Pavement - Brighten the Corners: Nicene Creedence ...
I Went to a Show: Best Kissers in the World at Sla...
Pavement - Wowee Zowee (2xLP, 1995)/Wowee Zowee: S...
Pavement - Crooked Rain, Crooked Rain: LA's Desert...
Pavement - Westing (By Musket & Sextant) (CD, 1993)
Pavement - Slanted and Enchanted (LP, 1992)/Slante...
Mike Patton - Pranzo Oltranzista (CD, 1997)
Mike Patton - Adult Themes for Voice (CD, 1996)
Park-Like Setting - School Day 2, Garbage Day 4 (C...
Paris - Acid Reflex (2xLP, 2008)
Paris - Sonic Jihad (CD, 2003)
Paris - Unleashed (CD, 1998)
Paris - Guerrilla Funk (CD, 1994)
600th Post: The Tide is Turning.
Paris - The Devil Made Me Do It - The Deluxe Editi...
Pailhead - Trait (CD, 1988)
Stallion Alert at the Movies: Deep Crates (2004)
Outkast - Idlewild (2xLP, 2006)
Outkast - Speakerboxxx/The Love Below (4xLP, 2003)
Outkast - Big Boi & Dre Present... Outkast (CD, 2001)
Outkast - Stankonia (2xLP, 2000)
Outkast - Aquemini (3xLP, 1998)


Colbert made his name as the longest-tenured correspondent on The Daily Show with Jon Stewart and later on his own Comedy Central show, The Colbert Report. Since 2015, he has been the Emmy and Peabody Award-winning host and producer of The Late Show with Stephen Colbert.
Bee, who is also an alum of The Daily Show, launched her own series, Full Frontal with Samantha Bee, in early 2016. In April 2017, she hosted the gala "Not the White House Correspondents' Dinner" which countered the White House Correspondents' Dinner. The event raised $200,000 for the Committee to Protect Journalists.
Both comedians have been extremely critical of Donald Trump's presidency, using the politic landscape as a primary topic for their respective shows. Expect their on-stage discussion to address White House politics and other pressing current events.
This event is made possible with generous support from NorthJersey.com. For tickets and all event information, visit the NJPAC website.


text:
Share this Story: An organic farmer's long road from conventional to 'now'
An organic farmer's long road from conventional to 'now'
Jun 24, 2014 • June 24, 2014 • 6 minute read
Tammy Van Troost is an organic farmer and president of the Lambton Local of the National Farmers Union.
She and her husband, Peter, farm 156 acres near Bridgen, Ontario and raise beef cattle, corn, soybeans, oats and wheat.
She also has a small market garden where she grows and sells mostly heritage variety vegetables to local customers.
"We are a mixed farm and don't market any one specific commodity," she says.
"We have our eggs well spread out into many baskets."
Speaking at an information meeting held recently at the Petrolia Library, Van Troost said she wasn't always an organic farmer.
"We were conventional like most everyone else," she said, adding that when they began farming they accepted that all this new technology was safe, otherwise it would not have received government approval.
"Like most everyone else, we jumped on the bandwagon believing it was safe for our environment, our livestock and ourselves."
She added that they also believed that there had been long-term testing of Genetically Modified Organisms (GMO's).
"We found out later that there has never been any long-term testing of these products," she said.
She noted that in the 1990s when farmers were first introduced to GMO technology, the companies behind them promised it would provide higher yields with the use of fewer chemicals and would increase a farmer's bottom line.
"At the time farming was a tough go and the bottom line was an important thing," she said.
"We slowly adapted and grew GMO crops such as Roundup Ready soybeans and Bt corn and I admit we were ignorant and didn't know what genetic modification really was, I thought it was just select breeding, which it is not."
She added that she soon discovered that this technology was geared for large industrial farms.
"It was not designed with the typical family farm in mind," she said.
Nevertheless, she said they accepted all the hype around the new technology and after growing them for several years found not much happened in terms of all the promises made.
"We did get a little better yield but there was no less need for commercial fertilizer, herbicides and pesticides," she said.
However, she said they did notice other things were happening on their farm.
"We now had super weeds that became resistant to the chemicals we were using as well as pressure from new weeds and pests that didn't have before," she said, adding that they also had an imbalance in their soil's nutrients and later found 90 per cent of weed issues are caused by soil imbalances.
But the biggest issue for them at the time was that their so-called bottom line was not any better.
"When we got our crops off in the fall and delivered them to the elevator we basically traded cheques to cover the input costs," she said.
Became a label reader
Van Troost said they started their family in 1997 and their first daughter, Jesse, was allergic to iron-fortified foods as a baby.
"Consequently I became a label reader and as she grew up it became a habit and I started to realize there were a lot of things in our food that I had no idea what they were," she said.
She said as a food grower that kind of shocked her because the names listed on food cans and boxes was not what she was growing and this started to raise a lot of questions.
"I thought if I can't pronounce it, what the heck is it?" she said, adding that as she researched these ingredients she found that there very few of them that started out in the soil.
She said it was about that time when she came across a book titled The End of Food by Thomas Pawlick and later attended a seminar at which he was speaking.
"I verified all his facts and the more I read, the less I wanted to eat I wanted to eat what I was growing and as a result I decided to investigate alternative farming practices," she said.
"We started to investigate organic production because a lot of the stuff we were doing, I didn't see as safe and If I wasn't willing to eat it myself, there is no way I was going to put it on the market for others," she said, adding that further investigation brought to light issues, not only for their own health but for that of their livestock, soil ecology and the impact on their local environment, not to mention their suffering bottom line from buying costly crop inputs.
Finally, she said they decided to make the transition to organic farming.
They paid the fees, submitted to a rigorous inspection and auditing process, and refrained from using commercial fertilizers, herbicides and pesticides.
In generally, she said they found the three-year transition period required to become certified organic, a very steep learning curve.
"It's almost like a cleansing period for your soil," she said.
"I still find that every day I learn something new and some days it's an overwhelming amount."
Considers seeds a gift from God
Van Troost said they also adopted the long-held practice of selective seed saving.
She noted that for centuries farmers fed their families by growing crops and selectively saving their own seed for the next year's crop.
She pointed out that they didn't save the poor stands which were adversely affected by drought, excessive rain, pests or disease.
"They saved the best seed for the next crop," she said.
"They saved seed that had demonstrated a natural adaption to their local environment and soil conditions."
She added that in the process they learned which crops were suited for their particular soil type and which were better suited for drier or wetter areas.
"There was definitely heritage in the seeds they saved and as a result their farms were in balance with their environment," she said.
She said the biggest benefit of this tradition was that the seed belonged to the public or the common people, who were free to share, trade or sell them, there was no patented ownership of the seed.
"I have always believed that seeds are a gift from God to all of us, not just a select few," she said.
"They are meant for all of us that we might be able to sustain ourselves. I also believe God gave us a balanced soil to grow those seeds and I need to do my part in protecting what He gave us."
GMOs place food sovereignty and environment at risk
Van Troost said the movement to GMO technology and global production is puts a nation's food sovereignty and environment at risk.
She said the term Genetically Modified Organism or GMO is used to refer to any micro-organism, plant or animal, essentially any living thing in which genetic engineering has been used to introduce, remove or modify specific parts of its genome or DNA.
"This means to alter what God has made and given to us as a gift," she said.
"I don't believe God made all these things for humans to tinker with."
Van Troost said a mere six companies now control 60 per cent of the world's seed supply and more than 70 per cent of the chemicals used in production agriculture today.
"Farmers pay royalties to these companies on nearly every seed they plant and they cannot keep any of them for future crops," she said.
"We will soon lose our right to save seed at all, every seed will patented and belong to someone and that is my greatest fear," she said.
An organic farmer's long road from conventional to 'now' Back to video


This hotel courtyard has been transformed into a sheltered green oasis using Elmich VGM 150 greenwall system. The thousands of plants used to create the walls insulate the courtyard from the sounds of the nearby city, keeping the location peaceful.
VGM contain a geotextile liner into which is placed a suitable planting mix. The modules are preplanted in a nursery environment to allow proper establishment to occur before installation on site.
VGM are either mechanically fastened on walls using steel bolts or inserted into free standing steel support racking structures.
VGM installations include drip irrigation systems that are positioned at appropriate intervals, depending on wall heights. Collection trays may be positioned, at ground level to allow overflow water to be discharged or recycled.


text:
NBA pro basketball player Rui Hachimura's third signature model
This watch is designed with a motif based on the Tateyama mountain range in Hachimura's home prefecture of Toyama. The band boasts mountain graphics, and the dial is printed with a contour map. Hachimura's signature "Black Samurai" logo is featured throughout.
RUI HACHIMURA COLLABORATION MODEL
DW6900RH-2D
Hachimura began playing basketball in earnest in middle school. While at Meisei High School in Miyagi Prefecture, he led his team to three consecutive victories in the All-Japan High-School Tournament.
While still a student, he was selected as a candidate to play for Japan's national team.
In 2016, Hachimura attended Gonzaga University in the U.S., a school with a highly respected basketball program in the National Collegiate Athletic Association (NCAA). In his third season as a key player, the Gonzaga Bulldogs made it to the Elite Eight in the NCAA tournament, and he won the Julius Erving award as the best small forward that season.
In 2019, Hachimura became the first Japanese national ever to be taken in the first round of the NBA draft, and joined the Washington Wizards. He played in 48 of 72 games his rookie season, and his stellar performance earned him a spot on the second-team NBA All-Rookie Team.
Bezel and Band Design
A graphic representation of the Tateyama mountain range, symbol of Hachimura's home prefecture of Toyama, adorns the band. The bezel incorporates light-blue translucent resin to evoke the abundant water resources found there. The light-blue printing on the white band represents the mountain range's majestic snow-capped peaks.
Dial Design
The dial is printed with a contour map of the Tateyama mountain range. The name "RUI HACHIMURA" is paired with the G-SHOCK logo engraved into the translucent bezel.
Hachimura's signature "Black Samurai" logo is laser-engraved on the case back. The symbol 八 (hachi in Japanese, meaning "eight") represents both his name and jersey number. The design incorporates a Japanese sword that crosses the 八 hachi symbol, resulting in an additional "H" motif for "Hachimura."


It is inevitable. Time passes and we get older.
Depending on many factors, including heredity, mental and physical health, exposures to certain agents in the environment and occupations, our bodies will have some level of decline.
Some of us will be able to continue to live independently, but for others that no longer is an option.
Don't wait for a crisis situation to act. Prepare now.
There are ways to plan for changes coming, like talking to a qualified licensed insurance agent about long term care insurance. For some, if skilled care is later needed, this benefit can bridge the gap until you become eligible for other benefits.
Policies differ and it may take an attorney to decipher all of the legal terms in your long term care insurance contract. Do not assume your policy covers something if you have not reviewed it with an attorney.
Also, before it becomes a crisis situation, you can plan ahead for the possibility of skilled nursing care by legally protecting your assets. The federal government has issued laws and regulations on "look back periods" for the transfer of assets and qualification for Medicaid benefits.
With proper pre-planning, and in accordance to the rules Congress has given us, you can legally shelter some assets, if you timely act. That way you are ensuring they pass down to your family in the manner you decide. Which is why you worked so hard isn't?
Please give us a call at 502-805-1133.


text:
/*
 * DO NOT EDIT.  THIS FILE IS GENERATED FROM e:/builds/moz2_slave/rel-2.0-xr-w32-bld/build/accessible/public/nsIAccessibleProvider.idl
 */

#ifndef __gen_nsIAccessibleProvider_h__
#define __gen_nsIAccessibleProvider_h__

#ifndef __gen_nsISupports_h__
#include "nsISupports.h"
#endif

/* For IDL files that don't want to include root IDL files. */
#ifndef NS_NO_VTABLE
#define NS_NO_VTABLE
#endif

/* starting interface:    nsIAccessibleProvider */
#define NS_IACCESSIBLEPROVIDER_IID_STR "ac0639d5-f95b-4e2b-970c-9eab281fb6a5"

#define NS_IACCESSIBLEPROVIDER_IID \
  {0xac0639d5, 0xf95b, 0x4e2b, \
    { 0x97, 0x0c, 0x9e, 0xab, 0x28, 0x1f, 0xb6, 0xa5 }}

/**
 * nsIAccessibleProvider interface is used to link element and accessible
   object. For that XBL binding of element should implement the interface.
 */
class NS_NO_VTABLE NS_SCRIPTABLE nsIAccessibleProvider : public nsISupports {
 public:

  NS_DECLARE_STATIC_IID_ACCESSOR(NS_IACCESSIBLEPROVIDER_IID)

  /**
   * Constants set of common use.
   */
/** Do not create an accessible for this object
   * This is useful if an ancestor binding already implements nsIAccessibleProvider,
   * but no accessible is desired for the inheriting binding
   */
  enum { NoAccessible = 0 };

  /** For elements that spawn a new document. For example now it is used by
    <xul:iframe>, <xul:browser> and <xul:editor>. */
  enum { OuterDoc = 1 };

  /**
   * Constants set is used by XUL controls.
   */
  enum { XULAlert = 4097 };

  enum { XULButton = 4098 };

  enum { XULCheckbox = 4099 };

  enum { XULColorPicker = 4100 };

  enum { XULColorPickerTile = 4101 };

  enum { XULCombobox = 4102 };

  enum { XULDropmarker = 4103 };

  enum { XULGroupbox = 4104 };

  enum { XULImage = 4105 };

  enum { XULLink = 4106 };

  enum { XULListbox = 4107 };

  enum { XULListCell = 4134 };

  enum { XULListHead = 4132 };

  enum { XULListHeader = 4133 };

  enum { XULListitem = 4108 };

  enum { XULMenubar = 4109 };

  enum { XULMenuitem = 4110 };

  enum { XULMenupopup = 4111 };

  enum { XULMenuSeparator = 4112 };

  enum { XULPane = 4113 };

  enum { XULProgressMeter = 4114 };

  enum { XULScale = 4115 };

  enum { XULStatusBar = 4116 };

  enum { XULRadioButton = 4117 };

  enum { XULRadioGroup = 4118 };

  /** Used for XUL tab element */
  enum { XULTab = 4119 };

  /** Used for XUL tabs element, a container for tab elements */
  enum { XULTabs = 4120 };

  /** Used for XUL tabpanels container element */
  enum { XULTabpanels = 4121 };

  enum { XULText = 4122 };

  enum { XULTextBox = 4123 };

  enum { XULThumb = 4124 };

  enum { XULTree = 4125 };

  enum { XULTreeColumns = 4126 };

  enum { XULTreeColumnItem = 4127 };

  enum { XULToolbar = 4128 };

  enum { XULToolbarSeparator = 4129 };

  enum { XULTooltip = 4130 };

  enum { XULToolbarButton = 4131 };

  /**
   * Constants set is used by XForms elements.
   */
/** Used for xforms elements that provide accessible object for itself as
   * well for anonymous content. This property are used for upload,
   * input[type="xsd:gDay"] and input[type="xsd:gMonth"] */
  enum { XFormsContainer = 8192 };

  /** Used for label element */
  enum { XFormsLabel = 8193 };

  /** Used for output element */
  enum { XFormsOutput = 8194 };

  /** Used for trigger and submit elements */
  enum { XFormsTrigger = 8195 };

  /** Used for input and textarea elements */
  enum { XFormsInput = 8196 };

  /** Used for input[xsd:boolean] element */
  enum { XFormsInputBoolean = 8197 };

  /** Used for input[xsd:date] element */
  enum { XFormsInputDate = 8198 };

  /** Used for secret element */
  enum { XFormsSecret = 8199 };

  /** Used for range element represented by slider */
  enum { XFormsSliderRange = 8200 };

  /** Used for select and select1 that are implemented using host document's
   * native widget. For example, a select1 in a xhtml document may be
   * represented by the native html control html:select */
  enum { XFormsSelect = 8201 };

  /** Used for xforms choices element */
  enum { XFormsChoices = 8208 };

  /** Used for xforms full select/select1 elements that may be represented by
   * group of checkboxes and radiogroup */
  enum { XFormsSelectFull = 8209 };

  /** Used for xforms item element that is used inside xforms select elements
   * represented by group of checkboxes */
  enum { XFormsItemCheckgroup = 8210 };

  /** Used for xforms item element that is used inside xforms select1 elements
   * represented by radio group */
  enum { XFormsItemRadiogroup = 8211 };

  /** Used for xforms select1 element that is represented by combobox */
  enum { XFormsSelectCombobox = 8212 };

  /** Used for xforms item element that is used inside xforms select1
   * elements represented by combobox */
  enum { XFormsItemCombobox = 8213 };

  /** Used for dropmarker widget that is used by xforms elements */
  enum { XFormsDropmarkerWidget = 8449 };

  /** Used for calendar widget that is used by xforms elements */
  enum { XFormsCalendarWidget = 8450 };

  /** Used for popup widget that is used by xforms minimal select1 elements */
  enum { XFormsComboboxPopupWidget = 8451 };

  /**
   * Return one of constants declared above.
   */
  /* readonly attribute long accessibleType; */
  NS_SCRIPTABLE NS_IMETHOD GetAccessibleType(PRInt32 *aAccessibleType) = 0;

};

  NS_DEFINE_STATIC_IID_ACCESSOR(nsIAccessibleProvider, NS_IACCESSIBLEPROVIDER_IID)

/* Use this macro when declaring classes that implement this interface. */
#define NS_DECL_NSIACCESSIBLEPROVIDER \
  NS_SCRIPTABLE NS_IMETHOD GetAccessibleType(PRInt32 *aAccessibleType);

/* Use this macro to declare functions that forward the behavior of this interface to another object. */
#define NS_FORWARD_NSIACCESSIBLEPROVIDER(_to) \
  NS_SCRIPTABLE NS_IMETHOD GetAccessibleType(PRInt32 *aAccessibleType) { return _to GetAccessibleType(aAccessibleType); }

/* Use this macro to declare functions that forward the behavior of this interface to another object in a safe way. */
#define NS_FORWARD_SAFE_NSIACCESSIBLEPROVIDER(_to) \
  NS_SCRIPTABLE NS_IMETHOD GetAccessibleType(PRInt32 *aAccessibleType) { return !_to ? NS_ERROR_NULL_POINTER : _to->GetAccessibleType(aAccessibleType); }

#if 0
/* Use the code below as a template for the implementation class for this interface. */

/* Header file */
class nsAccessibleProvider : public nsIAccessibleProvider
{
public:
  NS_DECL_ISUPPORTS
  NS_DECL_NSIACCESSIBLEPROVIDER

  nsAccessibleProvider();

private:
  ~nsAccessibleProvider();

protected:
  /* additional members */
};

/* Implementation file */
NS_IMPL_ISUPPORTS1(nsAccessibleProvider, nsIAccessibleProvider)

nsAccessibleProvider::nsAccessibleProvider()
{
  /* member initializers and constructor code */
}

nsAccessibleProvider::~nsAccessibleProvider()
{
  /* destructor code */
}

/* readonly attribute long accessibleType; */
NS_IMETHODIMP nsAccessibleProvider::GetAccessibleType(PRInt32 *aAccessibleType)
{
    return NS_ERROR_NOT_IMPLEMENTED;
}

/* End of implementation class template. */
#endif

#endif /* __gen_nsIAccessibleProvider_h__ */

redpajama_set_name: RedPajamaGithub


There is evidence in the literature that viable cryopreserved human placental membrane (vCHPM) grafts are effective in treating diabetic foot ulcers and venous leg ulcers.
Objective. This case series presents 3 cases of chronic ulcerations — 1 arterial ulcer (AU), 1 pressure ulcer (PU), and 1 recurrence of a pyoderma gangrenosum ulcer (PGU) — that had failed previous courses of standard wound care and were subsequently treated with vCHPM to determine if the treatment is an effective modality for treating wounds of these etiologies.
Materials and Methods. This retrospective review describes 3 cases in which patients with chronic wounds that had failed standard of care treatments for more than 4 weeks were subsequently treated with weekly applications of vCHPM. Each wound area was recorded and photographed on a weekly basis and wound area reduction also was charted weekly.
← Inlow's 60-Second Diabetic Foot Screen Gets a New Look!


Market Urbanism is returning to partner with the Foundation for Economic Education to present an entire track of six sessions focused on Market Urbanism at the second annual FEEcon Conference.
Wherever you live, your city uses regulations to restrict what can be built and for what purposes buildings can be used. FEEcon's Urbanism, Development, & Your Neighborhood track is a joint effort by Market Urbanism and FEE to shed light on the vast spectrum of land use and transportation regulations that often diminish neighborhood communities, cause traffic congestion, and constrain housing supply to create affordable housing crises across the world. This track provides you with the intellectual tools you'll need to make a case for liberty in your own backyard.
FEEcon is the premier gathering of freedom lovers from all walks of life, with professional networking opportunities, inspiring panel discussions, and fun for everyone – all sponsored by FEE and held at the landmark Hyatt Regency Atlanta.
Choose from 50+ sessions and 8 distinct learning tracks all designed to provide real skills for professional success, combined with a solid grounding in economic, ethical and legal principles that you won't get anywhere else.
FEEcon will inspire and empower you to set your path and change the world!
FEEcon will run from Thursday evening, June 7th, through Saturday evening, June 9th, 2018. All events are at the gorgeous Hyatt Regency in downtown Atlanta.
Sandy Ikeda is a professor of economics at Purchase College, SUNY, and the author of The Dynamics of the Mixed Economy: Toward a Theory of Interventionism. Sandy publishes his blog, Culture of Congestion at Market Urbanism.
Adam Hengels is founder of Market Urbanism, which advocates for liberalization of land-use regulation and market-based transportation systems. He is also co-founder of Parafin, an artificial intelligence platform for real estate development.
Emily Hamilton is a Research Fellow for the State and Local Policy Project at the Mercatus Center at George Mason University. Her research focuses on urban economics and land-use policy.
Nolan Gray is the policy director for the Center for Market Urbanism and is a grad student in city & regional planning at Rutgers University. His areas of expertise include land-use regulation, development, and urban planning theory.
Anthony is currently an MBA Candidate at Stanford GSB, and editor of Caos Planejado, a Brazilian website covering issues on cities and urbanism.
Jeff is a technologist who co-founded Tech for Housing, a policy advocacy organization dedicated to rallying Bay Area tech workers around urban reform.
Michael Lewyn is a Professor of Law at Tuoro College. His scholarship focuses on urban and suburban development, and in particular the question of "sprawl".
The full lineup of FEEcon speakers can be found here.
Zoning is justified in all sorts of ways today, but at its birth—arguably in New York City, in 1916—it was aimed squarely at halting what upper-class New Yorkers saw as the decay of the city as neighborhoods built for the rich filtered down to the city's growing immigrant masses. A century later, the movement is in the other direction—the rich are outbidding middle-class and poor New Yorkers for space in a phenomenon known as gentrification. New Yorkers tend to view development as the cause, but a more careful reading of history shows that it's zoning, and the housing shortage that it's created, that are responsible for the reversal and for the growing waves of displacement washing over cities from New York to San Francisco.
Jane Jacobs famously argued that "a city cannot be a work of art." Rather, a city is a place where people with diverse knowledge, skills, and tastes change space, make and break ties, and transform resources and ideas in innovative and controversial ways. It's an unpredictable, messy—even dangerous—but deeply creative process.
Why are young people and immigrants struggling to afford to live in your city? It's simple supply and demand, and decades of government policy at multiple levels is making matters worse.
Capitalism was and is the great prosperity engine behind all the material freedoms of modern life. Tragically capitalism is not allowed to work its magic with what matters most to us, namely our dwellings and cities. Urban development and housing provision have been unduly politicised and thereby paralyzed. We should be experiencing an urban Renaissance as crucial productivity boosting component of our knowledge-and network society. Instead planning restrictions and imposed standards block the adequate supply of urban residences leading to prohibitive prices. Paradoxically, the affordability system contributes to rather than alleviates the affordability crisis.
Mobility is one of the main factors that explains the productivity of large cities. Urban transport policy's main objective should be to increase mobility, i.e. to decrease commuting time by increasing travel speed. Too often transport policies rely on anticipated utopian land use changes to justify the design of a preferred transport mode. Increasing mobility becomes then only a secondary objective.
Public and Private transportation in the past, present and future. How economics and transportation shapes the places we live.
If you're flying, plan to arrive at Hartsfield-Jackson Atlanta International Airport (ATL). FEEcon will be held at the Hyatt Regency Atlanta located on 265 Peachtree St NE, Atlanta, GA 30303. There will be a room block available at the Hyatt, and there are numerous other lodging options nearby. The Hyatt has valet parking accessible from Peachtree Road and is conveniently located directly next to the Peachtree Center MARTA Station.
More information, including FAQ can be found at the FEECon website.


The American household is not quite complete without a good-quality blu-ray player. People take the trouble of going through dozens of reviews, product catalogues and manufacturer information, if only to find the best 3D blu ray player 2019. A blu ray player gives better viewing quality. It is able to play not just standard DVDs and CDs but blu ray discs as well. Premium blu ray players have WiFi connectivity, built-in internet apps, dual HDMI and various audio outputs and also HDMI inputs. You don't have to go over complicated literature to score the best deals on 3d blu ray players as I have described in the following paragraphs the best products in this category.
In the beginning, people were skeptical about how well the Blu-ray technology would fair, but now it is safe to say that Blu-Ray has become one of the most popular ways people consume movies. Because of this, there are a slew of players out on the market and you may think a cheap 3D Blu-Ray player will work as good as a more expensive model. Unfortunately, that is not the case. We have created this buying guide to help you recognize the features you should look for.
A new 3D Blu-Ray player is an excellent way to round out your home theater system, especially if you have a HD 3D television. Your player should display high-quality 1080p images in 3D with no problem. The player should feature 24p Cinema and Deep Color. The movies that you see in theaters are shown in 24p and that refers to the frame rate per second. This gives you a smoother picture while watching. Deep Color refers to the richness of the color and is usually used in movie theaters. With a 3D player, these technologies can be viewed at home.
The highest rated 3D Blu-Ray players feature high tech audio technology like Dolby TrueHD, DTS-HD and LPCM. These technologies put DVD players and their sound integration to shame, as the latest technologies boast to have movie studio quality at 24.5 Mbit/s when compared to non-3D Blu-Ray players, which use 18 Mbit/s.
When you are trying to decide which is the best player for your theater system, you want to look at the extra features. Some devices feature Wi-Fi connectivity or BD-Live. Other players can connect to your smartphone via an app and it can turn your phone into a remote control. While some may feel that this particular feature is a gimmick, it can be a useful tool, especially if you happen to lose your remote control! Other players use that Wi-Fi connectivity to grant you access to their own app store. There, you can find some of the top ten streaming apps for movies, so not only are you able to watch 3D movies, but the latest releases too.
Chances are that if you have a 3D player, you are probably tech minded and have other media players. You will want to find a player that has the ability connect to all of your other devices. The higher end of players feature the fastest HDMI ports and have the capability to connect to older devices that use component, composite and coaxial ports. Since portable media is also a popular way of media consumption, you may want to make sure the player has USB ports and S-video options so that you can hook up your computer, flash drive, or a tablet.
We hope that this guide was able to shed some light on 3D Blu-Ray players and some of the key features that you want to look for when purchasing one.
Look for a device that can display 1080p as well as featuring 24p Cinema and Deep Color. These features will give you the best picture that you would expect from a high-definition player.
The player should produce theater quality audio, which is 24.5 Mbit/s. Look for technology like Dolby TrueHD, DTS-HD or LPCM.
Make sure your device can connect to all the other kind of home theater devices you may own. The more ports, the better!
Every form of TV entertainment instantly transforms to advanced 3D Entertainment with the Samsung BD-H5900 Blu-ray Player. It has built-in WiFi that lets you connect to the web with ease. Delight in a growing library of Built-in Apps exclusively from Content Partners + Opera TV Apps Store. There is always something new to be enjoyed on TV as you can watch blockbuster titles and even new releases via streaming entertainment. The BD-H5900 has 1 USB 2.0 output and 1 HDMI output for added versatility. Furthermore, it has state-of the-art HD Up-conversion that auto-enhances non-HD video to near-high def quality.
No DVD disc is ever ordinary when it is played on the best 3D blu ray players 2016, particularly the Samsung BD-H6500 3D Blu-Ray Disc Player. Change the way you look at TV viewing and step up your entertainment experience. This blu ray player does UHD up-scaling so every disc is rendered in near full high definition clarity. Apps that are built for TV are available to you 24 hours a day. Your favorite content gets directly streamed to your TV in superb 3D detail. With the legendary Samsung Smart Hub, you can explore shows, newly released and classic cinema masterpieces, social media and apps all in one easy-to-use hub.
Wonder no more how full definition 1080p feels like. Just get yourself the LG Electronics BP540 3D Blu-Ray Disc Player and realize that there's always more to TV than meets the eye. This disc player is capable of playing both 2D and 3D blue-ray movies in near high definition quality. With LG Electronics' Smart TV Interface, you can get access to a wide variety of internet apps and content including those from Vudu, Netflix, YouTube and Amazon Instant Video. The BP540 3D Blu-Ray Disc Player has built-in WiFi to make all that possible.
With built-in WiFi and an award-winning design, the Sony BDP-S5100 3D Blu-ray Disc Player has all the bells and whistles to make it one of the best 3D blu ray players 2019. Enjoy astoundingly high definition blu-ray disc playback of 1080p quality with conversion from plain 2D to revolutionary 3D. Once you've experienced the TV SideView feature on the Sony BDP-S5100 for browsing and controlling with your mobile devices, you will never look back-ever! This player has I/P noise reduction and enclosed drive so images are always clear, brilliant and captivating.
Basic DVDs get upgraded to near HD quality with the LG Electronics BP335W 3D Blu-Ray Disc Player, simply the best 3D blu ray player 2019 for millions of blu-ray enthusiasts. You can take pleasure in watching hours of 3D Blu – ray Disc movies in Full HD 1080p and standard Blu – ray Disc movies in high definition. This blu-ray player has Wi-Fi as well as integrated Premium Internet Services. With good Internet access, you can seamlessly stream content from online sites like Vudu and Netflix straight to your TV, with no computer required. With less clutter and infinite possibilities at your fingertips, TV viewing has become more interesting!


text:
Samuel Watkins Eager (April 8, 1789 – December 23, 1860) was a U.S. representative from New York.

Born in Neelytown, New York, Eager attended Montgomery Academy in Montgomery, New York, and graduated from Princeton College in 1809.
He studied law.
He was admitted to the bar in 1811 and commenced practice in Newburgh, New York.
He moved to Montgomery, New York, in 1826, and continued the practice of his profession.

Eager was elected as an Anti-Jacksonian candidate to the Twenty-first Congress to fill the vacancy caused by the resignation of Hector Craig and served from November 2, 1830, to March 3, 1831.
He was not a candidate at the election held the same day for the Twenty-second Congress.
He returned to Newburgh in 1836 and engaged in literary pursuits.
He died in Newburgh, New York, December 23, 1860.
He was interred in St. George Cemetery.

References

1789 births
1860 deaths
Princeton University alumni
National Republican Party members of the United States House of Representatives from New York (state)
People from Montgomery, New York
19th-century American politicians

redpajama_set_name: RedPajamaWikipedia


Gaint Iguana Disc. Hardtail. 2009-2010 model. Size=Medium.
SLX RD, deore FD and Shifters.
Have installed many new equipment after purchase.
New Rockshox Recon Air with adjustable rebound and lockout.
selling with Brand new in Package new 9 speed cassette: HG400-9 and sram PC 971 chain.
Reason: bought new cassette and chain to install and ride.. total lack of time making me sell it.


Vets @ Acacia Gardens, Veterinary Surgeon, listed under "Veterinary Surgeon" category, is located at Cnr Park Road & Quakers Hill Parkway Quakers Hill NSW, 2763, Australia and can be reached by 0298375410 phone number. Vets @ Acacia Gardens has currently 0 reviews.
Browse all Veterinary Surgeon in Quakers Hill NSW.


CAMERA BASICS WITH DUSTIN WILLIAMS PHOTOGRAPHY!
So you got a New DSLR? That's Exciting! But umm… What do you do with it? Let me show you!
Everyone has to start somewhere, so why don't you allow me to help you with that? You could start by flipping through that 100+ page manual you get in your nifty cardboard camera box. How do you know what part of it actually pertains to you and what you need to know? In this workshop I will guide you through the aspects of your camera that you need to know. The parts that will make a difference in your photos, and have you feeling confident in your abilities. Be able to handle your camera, without hesitation.
*PLEASE NOTE - The Workshop will be held UPSTAIRS. Don't get confused when you walk into a downstairs office space!
So What Am I Going To Learn?
Any Nifty Perks For Attending?
Unlimited 24/7 365 day access to my Private, Informative, full of Classified Info Facebook Group. You will be able to interact with other workshop attendees. Post your new, amazing photos you will have taken after the workshop and receive feedback from myself, as well as other group members. Be in the know when I do group photo outings so you can tag along and get in the field guidance.
Giving away one print to one lucky person in attendance!
A complimentary bottle of water! You don't even have to bring your own!
Who Is This Dustin Williams Guy?
You know, that is a really great question. Half the time I'm still trying to figure out who I am myself. So let me just tell you a little about me and what I've done.
Most notably known as photographing the Milky Way here in Pensacola! I've actually been noticed in public! ISN'T THAT CRAZY?
Official Photographer for the former Double A affiliate Cincinatti Red Baseball Team, the Pensacola Blue Wahoos.
Featured on Buzzfeed, and several other news outlets! I went viral!
Featured in local shops, and restaurants.
Most importantly though, my great accomplishment isn't any of these things. My greatest accomplishment and proudest moment is when I see others that I've had a hand in helping succeed. Even more so than success myself. I have never seen the point acquiring knowledge if I can't use it to help others. That's who I am. That's what I hope to do for you.
"Super helpful (even though you shoot Nikon) your instruction was able to cross brands and still provide expert guidance. I learned so much in just shooting the night sky with you one time!
"Oh wow, how can I list ALL you've done for me in 4-5 sentences?! Seriously though, the 1st time I ever met Dustin was at Gulf Breeze Zoo. He was so excited about getting a new lens & offered to let me shoot with it. I couldn't believe what a kind-hearted person he was then & he continues to be a giver & a helper all the time! He patiently learned my camera (Canon) with me so he could answer all my multiple questions. He never says, "I've already taught you how to do that before" even when he's taught me the same things over & over!
Now You Know. What Next?
Now that you've read through this entire page, at least I hope you did, I hope I've been able to answer all your questions! What the workshop is about, what I'm about, how good of a journalist I am(not really) and so forth. If you've decided this is the workshop for you, the snazzy little button below will take you to the page to buy tickets. If for some reason you said "Nope, this ain't for me!" that's okay! Whether it be the day, time, wrong workshop for you, or so forth, that's okay! This is definitely not going to be the last workshop! There's many more where this one is coming from! I hope to see you on April 6th!


Absolute Write Water Cooler > Writing Genre > Bio, Autobio, and Memoir > Several ideas for short memoirs I wanted to run by you heady dudes.
View Full Version : Several ideas for short memoirs I wanted to run by you heady dudes.
I would just like to point out that when I read the essay you sent me, I was very intrigued by the brief mention of Karate For Christ.