Businesses and industry on Tasmania's north west coast are thriving, yet the economic conditions making this happen appear to be influenced by external market forces such as the Aussie dollar and overseas investment interests.
However, falling short is the mining industry on the north west coast, which has taken a hit in recent months due to international commodity prices. This has impacted heavily on local prospects, but many of us observing this have been around long enough to recognise that the worm will turn and mining will again rise to be the great economic contributor.
The next step for the Tasmanian mining industry is to re-manage the difficult and time-consuming approval processes, as we are still to take advantage of the depth of untouched resources available in our state. On a positive note, the fall of the Aussie dollar will strengthen the business case for many mines to either start up or re-open, and the mining industry will continue to be an economic strength in Tasmania for many decades to come.
The forestry industry continues to surprise us all, as new owners begin the onerous task of refiring past customers and markets. Hopefully the new ownership of Hampshire Woodchip will see the plant resume full production within a few months so harvesting can continue.
Despite political disputes, woodchip production is busy growing and is a major asset for the state. The fall in the Aussie dollar will generate significant demand for the immense resource and the stability of a majority government should enhance the investment climate, allowing long term contracts to be established again.
This is an amazing turnaround from a few short years back, recalling on the timber receiverships that did the economy no favours. However, the new owners of the Hampshire Woodchip plant seem to have hit the ground running.
Agriculture is in a season of positive outlook, with new potato contracts, incredibly popular beef that is now attracting premiums in some markets, and excellent dairy returns, producing favourable prospects for the future.
It has been a long held view that our food production is world recognised for its high quality and value, rather than just another commodity product on the world stage, and accordingly there are prospects for record returns for premium beef products in coming years.
The worlds demand for our food production will influence Tasmania's approach to agriculture for decades to come. This market outlook will create demand for more land to be converted to beef production; something that would have been unheard of in recent years. It is firmly believed that agriculture will continue to rise in its influence on Tasmania's economic future, and the case now exists to free up lots of unutilised land for higher and better agricultural use.
Tourism has had an amazing recovery from the doldrums of recent years and it is pleasing that this recovery is extending to the regions, including north west Tasmania.
Our hospitality industry has a long way to go and training and skill development will be required if we are to meet the future potential of this growing industry. Penalty rates are also a major inhibitor for business to invest the right funds for the opportunities that are presenting themselves.
Building and construction industries in the north west seem to be missing out on the boom currently being experienced in the south of the state. New buildings seem to be a great indicator of things to come and we have all experienced the boom created by the global financial crisis.
Unfortunately construction firms naturally build their workforce to cope with the boom times, only to have to make difficult choices when the industry backs off. It is to be hoped, that the changes to the Planning System, currently under discussion, will encourage a growth spurt in housing and construction. Also, the current prevailing interest rates present opportunities not previously experienced for many years.
The world of retail is changing at such a fast pace that it is difficult to see how the empty shops will be refilled. The informed purchaser has too many options to buy retail goods with the realities of the internet, and the past loyalties of shopping locally are not being embraced by the emerging shoppers.
Accordingly, retail in the north west remains subdued, in spite of a healthy Christmas trading season. However, smart retailers are changing their management operations to have some excellent internet presence, and I am amazed at the number of retail shops that are prospering in this environment. It's hard to imagine what our city and town streetscapes will look like in 10 years' time.
Investor confidence in Tasmania is growing. The visit by the Chinese President, Mr Xi Jinping, to Tasmania in November has sparked a frenzy of potential investment in Tasmania. The frenzy has not translated to much actual investment at this time, however, the potential for hundreds of millions of dollars, still remains.
The challenge we have is to tap into the billions of overseas investment dollars. My experience in Asian investment highlights that we are quite unprepared for what the investors are looking for. We have lots of great ideas, but no prospectus' that make it easier for investors to commit. Therefore, until we get the right prospectus development model right, we will continue to miss opportunity after opportunity.
Perhaps right sized councils will allow proper resourcing of the economic investment potential of each area. In my view, all councils need to have a capacity to develop prospectus to accommodate the enormous opportunities in their areas, with capable staff to assist development opportunities.


All writers have to learn the art of life balance, especially writers who are not ready to quit their day jobs, and especially-especially writers with young families. Let me tell you how it is, as the mom who finished a book when my daughter went to kindergarten (just like I always said I would) and who gardens with decorative vegetables (having given up on my home design Pinterest board and also my goals of growing organic produce that can actually feed my family).
Pictured below is our decorative corn plant. A local farmer has explained to us that it cannot grow actual corn due to its lack of fertilization partners, but it is reaching for the stars nevertheless. Cornspiration!
Also pictured: my beloved electric car, which can go no more than 70 miles round-trip on the best of days; a street sign that symbolizes how sometimes you have to slow down or stop and wait--so deep, man; my recycling and garbage bins with a utility company that uses the garbage stink gas to create electricity--also mega poetical; the interplay of light and shadow on the grime patina of my siding.
We writers and other artists, entrepreneurs, and self-employed workers have to be our own bosses. We set our own hours, hold our own professional boundaries, and manage our own risks. But that's not all. We also have to figure out how to not lose our everlovin' minds through the inevitable frustrations, delays, obstacles, and unforeseen sacrifices that come along with messy, unpredictable, and slow processes like raising kids and writing books.
You can have it all (work life and mom life). But the small print is that you cannot have things just the way you want.
This is essential, because no matter how hard we work at our craft and no matter how wisely and progressively we parent, there are many system dynamics that are beyond our control.
Sometimes that works out in our favor. Sometimes we find freedom, beauty, and inspiration in the chaos. That is the nature of art and living things.
In the photo above, a flower in the foreground wilts while the rose of sharon in the background sends forth its first bloom. I never know exactly when either of those things will happen, but I do know that they will happen--just like my daughter's growth and illnesses, achievements and failures, sweet moments and meltdowns.
And writing and marketing novels is no less of a long-distance mindgame.
I finished a novel when my daughter went to kindergarten, just like I said I would. But I haven't sold it. I've rewritten it several times. I've sent out about 25 queries total on its various iterations. I've attracted the interest of two awesome, top-tier agents. Each of them held the book in consideration for months before declining with kind and helpful rejections.
I rewrote the book again, fixing errors and strengthening the main character's arc and voice. But then, my last round of queries on the book's latest and greatest revision resulted in a slew of immediate form rejections. Around the same time, I noticed that some of the authors and agents whose careers I follow started finding difficulty in selling longish, fairy-tale-ish fantasy novels. I got the sense that I had narrowly missed a spike in demand for that sort of thing, which has since fizzled. So I shelved my finished work, The Grove of Thorismud.
That doesn't mean I've given up on it or that I won't ever query it again. But I have made the decision, while I can--that is, while I am still without a contract that holds me to official deadlines--to stop here and work on one novel at a time.
My new work in progress is in a different genre, historical fiction, which is one of my favorites to read. I'm having a great deal of fun researching and writing it, and I remind myself that I wouldn't be having all this fun right now if I had not made the decision to shelve my fantasy book for the time being.
Nor would I be enjoying the wonders of this amazing decorative corn plant if I had completed the design of my front garden bed and not left a space where my daughter could plunk in the seedling she started during her last days of kindergarten.
There is a freedom in work left unfinished and dreams deferred--a space where we can wait and see, discover the unexpected, savor simple joys, and be present for those fleeting moments that can't wait.
Maybe not the rat race, but is that really the goal here? I suspect that for those of us who chose, when we were first becoming our adult selves, to prioritize love and family and wandering explorations of humanity and beauty and art, that's a big, resounding NOPE.
Let's return to my decorative corn plant. Look at how tall and proud she has grown despite all of her life's limitations and setbacks.. She didn't get to choose where she was planted. She lives in a barren corner of concrete and asphalt, isolated from other corn plants who might have fertilized her. Is this the life she envisioned for herself when she was planted in a paper cup of soil in Ms. B's kindergarten class?
What grain of ambition has driven her to redirect all of her energy into the height of her stalk and the glory of her leaves after being told that she can never bear fruit?
SWEET HOLY MOTHER OF--WHAT IS THAT?
Um, congratulations, Ms. Single Lady!
Apparently Mama Corn has not accepted the advice of the farmer or awaited the services of a nearby partner. She has gotten down with her bad self... or colluded with a well-traveled bee... or prayed real hard... and there you have it.
And the circumstances do not have to be ideal for us to reach for the sky, bear fruit (of a living or creative nature), and seize the life we must have from the limited circumstances we find ourselves cornered within.
But remember, getting frustrated does not mean we cannot be grateful too. There's no shame in pushing against our boundaries, succumbing to those moments when we collapse in a soggy pile, or accepting help and support from others. Ms. Corn here has needed to be rescued several times from the ravages of storms and is now supported by a couple lengths of twine keeping her from falling over.
We can't help feeling frustrated sometimes, so don't waste any time feeling guilty about that. It happens to everyone who goes about doing hard stuff. We can have it all, though we can't generally have it the way we envision it when we start out. And that is the corny truth.


Ever wished you can be your own graphic artist? Design your own personalized Christmas cards this year with Canva! Tina from Truly Rich Mom sent us mommy bloggers a link to Canva, an online design platform. You can easily create your own designs for cards, documents, Facebook covers, presentations, blog graphics and more!
I went over to their site and I was very pleased with their interface. It is super easy! Just search for images, click, drag and drop. Put everything together and voila! You have a great looking graphic instantly! Here's a sample of a Christmas card for our family. There are so many designs to choose from. I had fun browsing through all of them!
This December, Canva will be donating $50 to a charity supporting Typhoon Yolanda for this post. They are also giving away $10 credit for my readers here. What are you waiting for? Hop on over to Canva!
Easy drag and drop user interface with plenty designs to choose from!
Create your own Christmas card in minutes.
Save your designs. It doesn't stop at cards. Create graphics for Facebook covers, blogs and more!


text:
\section{Introduction}
The perspectives of exploiting electron spin for information
processing in spintronic devices stimulated basic research of
spin-related phenomena.\cite{RMP_323} In order to take advantage
of traditional semiconductor technologies, the exclusive
application of electric fields to generate and manipulate a
nonequilibrium spin density is of particular interest. In this
respect, the spin-orbit interaction (SOI) provides an attractive
mechanism for the pure electric manipulation of moving spins in
nonmagnetic semiconductors. Unfortunately, the very same SOI
depends on the carrier momentum, which is randomized by elastic
and inelastic scattering. This momentum dependence of the coupling
leads to the dominant spin relaxation and dephasing in III-V
semiconductors known as Dyakonov-Perel relaxation
mechanism.\cite{Dyakonov} In general, however, details of spin
dephasing depend on the involved scattering mechanisms, the band
structure, and the crystal orientation (see Ref. \cite{JAP_073702}
and references therein).

An sizable anisotropy of the spin relaxation has been
theoretically predicted~\cite{PRB_15582,JPC_R271} for
semiconductor heterostructures grown along the [001] axis.
According to these studies, a large spin-relaxation anisotropy
should exist for the in-plane spin polarization. Moreover, under
the condition that the strengths of Rashba ($\alpha$) and
Dresselhaus ($\beta$) spin-orbit coupling constants become equal
($\alpha=\beta$), the anisotropy should be maximal. Based on this
observation a proposal for a novel spin-transistor device
\cite{PRL_146801} was put forward. Recent experimental data
provided strong evidence for a huge in-plane anisotropy of the
spin dephasing time in [001] GaAs/Al$_{x}$Ga$_{1-x}$As quantum
wells.\cite{PRB_033305,APL_112111,PRB_073309} The efficient
suppression of relaxation for spins aligned along the [110]
orientation in heterostructures with equal Rashba and Dresselhaus
SOI strengths is an important result that certainly stimulates
further progress in spintronics.

Other promising structures for spintronic applications are quantum
well samples grown along the [110] direction. Very long
spin-relaxation times on the order of nanoseconds were
experimentally demonstrated for the out-of plane spin polarization
in such heterostructures.\cite{PRL_4196,PRL_036603} This effect is
caused by the absence of Dyakonov-Perel spin relaxation in the
particular crystal direction.

The common physical origin for weak spin relaxation in [110]
quantum wells as well as in [001] heterostructures with
$\alpha=\beta$ is the presence of an spin-rotation symmetry in the
two-dimensional electron gas (2DEG).\cite{PRL_236601} This
symmetry is robust and leads to an infinite spin lifetime and a
persistent spin helix for an idealized model. The theoretical
explanation, which has recently been confirmed by
experiment,\cite{PRL_076604W} will initiate a number of further
studies in this field. It is the aim of this paper to contribute
to this development by treating weakly damped eigen-excitations of
the coupled spin-charge system subject to a constant electric
field. Our approach bears some similarities with a traditional
field in solid state physics namely the study of space-charge
waves in crystals.\cite{BuchPetrov1} The electric-field-mediated
excitations of the coupled spin-charge system are probed by a
simulated experimental set up, which provides the wave vector to
resonantly excite internal eigen-modes of the biased SOI coupled
2DEG. We focus on excitation mechanisms that exploit surface
acoustic waves.

\section{Basic Theory}
Our model is based on a Hamiltonian that describes conduction band
electrons in a III-V semiconductor quantum well grown in the [001]
direction, which is used to be the $z$ axis of the coordinate
system
\begin{equation}
H_0=\frac{\hbar^2\bm{k}^2}{2m}+\hbar\bm{\omega}_{\bm{k}}\cdot\bm{\sigma}.
\label{Hamil}
\end{equation}
The effective electron mass, the in-plane wave vector, and the
Pauli matrices are denoted by $m$, $\bm{k}$, and $\sigma_{i}$
($i=x,y,z$), respectively. The precession frequencies
$\bm{\omega}_{\bm{k}}$ are due to the SOI, which contain both
linear Rashba and Dresselhaus contributions
\begin{equation}
\bm{\omega}_{\bm{k}}^{R}=\frac{\alpha}{\hbar}(k_y,-k_x),\quad
\bm{\omega}_{\bm{k}}^{D}=\frac{\beta}{\hbar}(k_x,-k_y),
\end{equation}
with $\alpha$, $\beta$ being the respective spin-orbit coupling
constants. These vectors are also interpreted as a
momentum-dependent internal magnetic field that acts on the
carrier motion. The neglected cubic terms to the frequency vector
$\bm{\omega}_{\bm{k}}$ play only a secondary role in our study.
Throughout this work, it is assumed that the spin-orbit coupling
energy is much smaller than the Fermi energy $\varepsilon_F$. The
model is complemented by the inclusion of elastic scattering on a
short-range impurity potential characterized by the elastic
scattering time $\tau$.

To elucidate the peculiarities of the spin-orbit coupled 2DEG, the
coordinate system is rotated so that the [110] direction becomes a
coordinate axis ($k_{\pm}=(k_x\pm k_y)/\sqrt{2}\rightarrow
r_{\pm}=(r_x\pm r_y)/\sqrt{2}$). Along the spatial $r_{+}$ axis, a
constant electric field $E_0$ is applied. In addition, a surface
acoustic wave (SAW) with the wave number $K_{SAW}$ and frequency
$\Omega=v_{SAW} K_{SAW}$ ($v_{SAW}$ is the sound velocity) should
propagate in the same direction giving rise to an internal
electric field. The total electric field $E_{+}$ is expressed by
\begin{equation}
E_{+}(r_{+},t)=E_0+E_{SAW}\cos(K_{SAW}r_{+}-\Omega t)+\delta
E(r_{+},t),\label{Feld}
\end{equation}
is self-consistently calculated by taking into account the Poisson
equation
\begin{equation}
\frac{\partial\delta E(r_{+},t)}{\partial r_{+}}=\frac{4\pi
e}{\varepsilon}(F-n),\label{Pois}
\end{equation}
with $F$ and $n$ denoting the nonequilibrium and initially
homogeneous carrier density, respectively (the components of the
spin-density matrix $F_{\mu}$, ($\mu =1,2,3,4$) are defined as in
Ref.~\cite{PRB_205326}). $\varepsilon$ is the dielectric constant.
Due to the excitation conditions in Eqs.~(\ref{Feld}) and
(\ref{Pois}), all quantities are independent of the spatial
coordinate $r_{-}$ for an infinite 2DEG. Along the $r_{+}$ axis,
periodic boundary conditions are assumed.

All electric field components act both on the charge and spin
degrees of freedom leading to specific field-induced eigen-modes
of the spin-charge-coupled system. The appearance and excitation
of these modes is treated by drift-diffusion equations that are
obtained from a kinetic theory for the spin-density matrix. For
the given orientation of the constant electric field $E_0$ and the
SAW field, the set of equations decouples and takes the form
\cite{PRB_205326}
\begin{equation}
\left[\frac{\partial}{\partial t}-D\frac{\partial^2}{\partial
r_{+}^2} \right]F+\mu\frac{\partial E_{+}F}{\partial r_{+}}
-\frac{\hbar}{2m}K_{+}\frac{\partial F_{-}}{\partial r_{+}}
=0,\label{eq_F}
\end{equation}
\begin{equation}
\left[\frac{\partial}{\partial t}-D\frac{\partial^2}{\partial
r_{+}^2}+\frac{2}{\tau_{s-}} \right]F_{-}+\mu\frac{\partial
E_{+}F_{-}}{\partial r_{+}}
-\frac{2}{\tau_{s-}}\frac{F_{-}^{(0)}}{nE_0}\left[
E_{+}-\frac{2D}{\mu}\frac{\partial}{\partial r_{+}}\right]F=0,
\label{eq_Fm}
\end{equation}
\begin{equation}
\left[\frac{\partial}{\partial t}-D\frac{\partial^2}{\partial
r_{+}^2}+\frac{2}{\tau_{s+}} \right]F_{+}+\mu\frac{\partial
E_{+}F_{+}}{\partial r_{+}}-K_{+}\left(\mu
E_{+}-2D\frac{\partial}{\partial r_{+}}\right)F_{z}=0,
\label{eq_Fp}
\end{equation}
\begin{equation}
\left[\frac{\partial}{\partial t}-D\frac{\partial^2}{\partial
r_{+}^2}+\frac{2}{\tau_{s}} \right]F_{z}+\mu\frac{\partial
E_{+}F_{z}}{\partial r_{+}}+K_{+}\left(\mu E_{+}-2D\frac{\partial
}{\partial r_{+}}\right)F_{+}=G_z, \label{eq_Fz}
\end{equation}
where $F_{\pm}$ and $F_z$ denote the in-plane and out-of plane
nonequilibrium spin densities, respectively. $D$ is the diffusion
coefficient, $\mu$ the carrier mobility, and
$K_{+}=2m(\alpha+\beta)/\hbar^2$ a wave number constructed from
the spin-orbit coupling constants. In addition, we introduced the
spin-relaxation times
\begin{equation}
\frac{1}{\tau_s}=4DK^2,\quad
\frac{1}{\tau_{s+}}=\frac{\cos^2\varphi}{\tau_{s}},\quad
\frac{1}{\tau_{s-}}=\frac{\sin^2\varphi}{\tau_{s}}, \label{spints}
\end{equation}
with $K=m\sqrt{\alpha^2+\beta^2}/\hbar^2$. The angle $\varphi$ is
used to quantify the coupling constants according to
$\alpha/\sqrt{\alpha^2+\beta^2}=\cos(\varphi+\pi/4)$ and
$\beta/\sqrt{\alpha^2+\beta^2}=\sin(\varphi+\pi/4)$. For the
limiting cases of a pure Rashba and Dresselhaus model, we have
$\varphi=-\pi/4$ and $\pi/4$, respectively. When the SAW field is
switched off, the applied constant electric field $E_0$ induces a
homogeneous in-plane magnetization $F_{-}^{(0)}$ that is
calculated from
\begin{equation}
F_{-}^{(0)}=\sqrt{2}\frac{\cos^2\varphi}{\sin\varphi}\hbar K\mu
E_0\frac{dn}{d\varepsilon_F}.
\end{equation}
Taking into account the Einstein relation $\mu=eD d\ln
n/d\varepsilon_F$, this magnetization is expressed by the result
$F_{-}^{(0)}=\hbar K \mu E_0 dn/d\varepsilon_F$ (with
$K=m\alpha/\hbar^2$) for a Rashba model ($\beta=0$) that was
derived by Edelstein.~\cite{Edelstein} When the SOI coupling
strengths become equal ($\alpha=\beta$), the spin-relaxation time
$\tau_{s-}$ diverges so that the result for $F_{-}^{(0)}$ strongly
depends on the initial condition and/or additional spin relaxation
mechanisms quantified by the scattering time $\tau_{sp}$
($\tau_{s-}^{-1}\rightarrow \tau_{s-}^{-1}+\tau_{sp}^{-1}$). The
divergency is also circumvented in the ac
response.\cite{PRB_205326,IJMPB_4937} In all cases, the
field-induced in-plane magnetization disappears for
$\alpha=\beta$. In Eq.~(\ref{eq_Fz}), $G_z$ describes the uniform
generation of an out-of plane spin polarization by optical means
or by the application of a perpendicular constant magnetic field.

From Eqs.~(\ref{Pois}) and (\ref{eq_F}), an expression for the
total time-dependent charge current density $I(t)$ is obtained
\begin{equation}
j(r_{+},t)+\frac{\varepsilon}{4\pi}\frac{\partial \delta
E}{\partial t}=I(t), \quad j(r_{+},t)=e\mu E_{+}F-eD\frac{\partial
F}{\partial r_{+}}-\sqrt{2}\frac{\hbar K}{m}\cos\varphi eF_{-},
\label{jdef}
\end{equation}
which completes the set of basic equations necessary to study
electric-field-mediated effects in the spin-charge coupled 2DEG.
The drift-diffusion Eqs.~(\ref{eq_F}) to (\ref{eq_Fz}) decouple
into two sets of equations for the components $F$, $F_{-}$ and
$F_{z}$, $F_{+}$. Accordingly, the spin-charge coupling prescribed
by Eqs.~(\ref{eq_F}) and (\ref{eq_Fm}) is treated in the next
Section, whereas Eqs.~(\ref{eq_Fp}) and (\ref{eq_Fz}) are solved
in Section 4.

\section{Spin-charge coupling}
The solution of Eqs.~(\ref{eq_F}) to (\ref{eq_Fz}) is facilitated
by the fact that all quantities depend only on
$z=K_{SAW}r_{+}-\Omega t$. The derivative with respect to $z$ is
denoted by a prime. Introducing the dimensionless functions
$f=F/n$, $f_{\pm}=F_{\pm}/n$, and $f_z=F_z/n$ and the parameters
\begin{equation}
Y_{+}=\frac{E_{+}}{E_0}, \quad Y=\frac{\delta E}{E_0}, \quad
\Omega_E=\mu E_0 K_{SAW},\quad \frac{1}{\tau_M}=\frac{4\pi
e}{\varepsilon}\mu n, \quad \Lambda=\frac{DK_{SAW}}{\mu E_0},
\end{equation}
we obtain the following set of coupled ordinary differential
equations
\begin{equation}
-\Omega f_{-}^{\prime}-\Lambda\Omega_E
f_{-}^{\prime\prime}+\frac{2}{\tau_{s-}}f_{-}
+\Omega_E\left(Y_{+}f_{-}
\right)^{\prime}+\frac{2}{\tau_{s-}}f_{-}^{(0)}\left(Y_{+}f-2\Lambda
f^{\prime} \right)=0, \label{dichte1}
\end{equation}
\begin{equation}
-\Omega\tau_{M}Y^{\prime}+Y_{+}f-\Lambda
f^{\prime}-\sqrt{2}\frac{\hbar K}{m\mu E_0}\cos\varphi
f_{-}=\frac{I}{j_0},\quad \Omega_E\tau_{M}Y^{\prime}=f-1.
\label{dichte2}
\end{equation}
These equations are solved by applying perturbation theory with
respect to the SAW electric field $E_{SAW}$. When the SAW field is
absent ($E_{SAW}=0$), all quantities are independent of $z$ and we
obtain for the constant charge current density
\begin{equation}
I_0=j_0\left(1-\sqrt{2}\frac{\hbar K}{m\mu E_0}\cos\varphi
f_{-}^{(0)} \right), \label{I0}
\end{equation}
with $j_0=en\mu E_0$. The spin-induced contribution on the
right-hand side of this equation results from the homogeneous
in-plane magnetization $f_{-}^{(0)}$ that vanishes for a system
with equal Rashba and Dresselhaus coupling constants
($\alpha=\beta$).

To proceed, we calculate the stationary current contribution
$\delta I$ associated with the SAW electric field. This
time-independent current contribution arises from carriers that
are driven by the SAW. A similar current can also be generated by
a moving optical lattice in a photorefractive crystal. As a
periodic boundary condition along the $r_{+}$ axis is assumed, the
solution is searched for in the form of a Fourier series
$f(z)=n+\delta f(z)$, $\delta f(z)=\sum_{p}\exp(ipz)\delta f(p)$.
Taking into account the Fourier transformed version of
Eq.(\ref{jdef})
\begin{equation}
\frac{I}{j_0}\delta_{p,0}=-ip\Omega\tau_MY(p)+\sum
\limits_{p^{\prime}}Y_{+}(p-p^{\prime})f(p^{\prime}) -ip\Lambda
f(p)-\sqrt{2}\frac{\hbar K}{m\mu E_0}\cos\varphi f_{-}(p),
\end{equation}
we obtain
\begin{equation}
\frac{\delta I}{j_0}=\frac{Y_{SAW}}{2}\left[1-\sqrt{2}\frac{\hbar
K}{m\mu E_0}\cos\varphi f_{-}^{(0)} \right]\left[\delta
f(1)+\delta f(-1)\right], \label{ee}
\end{equation}
with $Y_{SAW}=E_{SAW}/E_0$. The nonequilibrium fluctuation of the
charge density $\delta f(1)$ for $p=1$ is expressed by the
variation of the internal electric field $\delta Y(1)$ via $\delta
Y(1)=-i\delta f(1)/(\Omega_E\tau_M)$. The latter quantity is
calculated from the Fourier transformed Eqs.~(\ref{dichte1}) and
(\ref{dichte2}), which are given by
\begin{eqnarray}
&&
\left[-ip(\Omega-\Omega_E+ip\Lambda\Omega_E)+\frac{2}{\tau_{s-}}
\right]\delta f_{-}(p)\label{e1}\\
&&+f_{-}^{(0)}\left[ip\Omega_E+\frac{2}{\tau_{s-}}\left(1+ip\Omega_E\tau_M
\right) \right]\delta
Y(p)+4p^2\frac{\Lambda}{\tau_{s-}}f_{-}^{(0)}\delta
Y(p)\nonumber\\
&&=-\frac{1}{\tau_{s-}}f_{-}^{(0)}Y_{SAW}(\delta_{p,1}+\delta_{p,-1})-\frac{i\Omega_E}{2}
f_{-}^{(0)}Y_{SAW}(\delta_{p,1}-\delta_{p,-1}),\nonumber
\end{eqnarray}
\begin{eqnarray}
&&\left[1-ip\tau_M(\Omega-\Omega_E(1-ip\Lambda)) \right]\delta
Y(p)-\sqrt{2}\frac{\hbar K}{m\mu E_0}\cos\varphi\delta
f_{-}(p)\nonumber\\
&&=-\frac{1}{2}Y_{SAW}(\delta_{p,1}+\delta_{p,-1}). \label{e2}
\end{eqnarray}
Even at the absence of SOI, the SAW field alone gives rise to a
charge current that is easily calculated from Eqs.~(\ref{e1}),
(\ref{e2}), and (\ref{ee})
\begin{equation}
\left(\frac{\delta I}{j_0}\right)_1=\frac{Y_{SAW}^2\Omega_E}{2}
\frac{\Omega-\Omega_E}{(\Omega-\Omega_E)^2+(\tau_M^{-1}+DK_{SAW}^2)^2}.
\label{jSAW}
\end{equation}
This current contribution is due to space-charge waves, the
dispersion relation of which is obtained from the poles in
Eq.~(\ref{jSAW})
\begin{equation}
\Omega=\mu E_0K_{SAW}- i\left(\frac{1}{\tau_M}+DK_{SAW}^2 \right),
\end{equation}
where $\tau_M$ denotes the Maxwellian relaxation time. The
physical origin of this mode, which has been thoroughly studied in
the field of photorefractive materials~\cite{BuchPetrov1}, are
oscillations of the free electron gas. In the same way as the
current density $j_0$ has a spin complement in Eq.~(\ref{I0}), the
well-known SAW-induced charge current in Eq.~(\ref{jSAW}) has a
related spin contribution, which is also calculated from
Eqs.~(\ref{ee}) and (\ref{e1}), (\ref{e2}) with the result
\begin{eqnarray}
&&\left(\frac{\delta
I}{j_0}\right)_2=\frac{\hbar}{4m}\frac{K_{+}K_{SAW}f_{-}^{(0)}Y_{SAW}^2}
{\left[(\Omega-\Omega_E)^2+\left(\tau_M^{-1}+DK_{SAW}^2 \right)^2
\right]\left[\left(\Omega-\Omega_E
\right)^2+\left(2/\tau_{s-}+DK_{SAW}^2 \right)^2
\right]}\nonumber\\
&&\times\Biggl\{(\Omega-\Omega_E)
\left(\frac{2}{\tau_{s-}}+DK_{SAW}^2 \right)
\left(\frac{2}{\tau_{s-}}-\frac{1}{\tau_M} \right)\label{jend}\\
&& +\Omega\left[\left(\frac{1}{\tau_{M}}+DK_{SAW}^2
\right)\left(\frac{2}{\tau_{s-}}+DK_{SAW}^2 \right)-
\left(\Omega-\Omega_E \right)^2 \right]\Biggl\}.\nonumber
\end{eqnarray}
The SAW-induced electronic current in Eq.~(\ref{jSAW}) is
independent of the spin-degree of freedom and disappears at the
resonance frequency $\Omega=\Omega_E$ of space-charge waves. This
result has to be compared with Eq.~(\ref{jend}) that holds for the
spin complement of the SAW-induced charge current, which may
exhibit a sharp resonance at $\Omega=\Omega_E$. Besides
space-charge excitations that also appear in Eq.~(\ref{jSAW}),
there exists a new eigen-mode, in which $\tau_M^{-1}$ is replaced
by the spin-scattering rate $2/\tau_{s-}$ that vanishes for
$\alpha=\beta$. This spin-mediated mode has the character of a
space-charge wave with an infinite Maxwellian relaxation time (for
$\alpha=\beta$). In experiment, the SAW related stationary charge
currents in Eqs.~(\ref{jSAW}) and (\ref{jend}) can be
distinguished by their qualitative different dependence on the
electric field $E_0$.

\section{Spin-spin coupling}
For the considered set-up not all four components of the
spin-density matrix couple to each other. According to the special
field orientation, the coupling between the spin components $F_z$
and $F_{+}$ is separated from the charge density $F$ and the
in-plane spin component $F_{-}$. The related drift-diffusion
Eqs.~(\ref{eq_Fp}) and (\ref{eq_Fz}) take the dimensionless form
\begin{equation}
-\Omega f_{+}^{\prime}-\Lambda\Omega_E
f_{+}^{\prime\prime}+\frac{2}{\tau_{s+}}f_{+}
+\Omega_E(Y_{+}f_{+})^{\prime}-\frac{K_{+}\Omega_E}{K_{SAW}}Y_{+}f_z
+2\frac{K_{+}\Omega_E\Lambda}{K_{SAW}}f_z^{\prime}=0, \label{b1}
\end{equation}
\begin{equation}
-\Omega f_{z}^{\prime}-\Lambda\Omega_E
f_{z}^{\prime\prime}+\frac{2}{\tau_{s}}f_{z}
+\Omega_E(Y_{+}f_{z})^{\prime}+\frac{K_{+}\Omega_E}{K_{SAW}}Y_{+}f_{+}
-2\frac{K_{+}\Omega_E\Lambda}{K_{SAW}}f_{+}^{\prime}=\frac{G_z}{n},
\label{b2}
\end{equation}
where $G_z$ denotes the source of an out-of-plane spin
polarization. Without the application of the SAW field, we obtain
the steady-state solution
\begin{equation}
f_{z}^{(0)}=\frac{G_{z}/n}{2/\tau_{s}+(\mu E_0)^2/D},\quad
f_{+}^{(0)}=-\frac{\mu E_0}{DK_{+}}f_{z}^{(0)}.\label{fz0}
\end{equation}
The out-of-plane spin polarization $f_z^{(0)}$ is suppressed by
the electric field.\cite{Kalevich} By determining this suppression
in experiment, the spin-relaxation time $\tau_s$ can be determined
in a way similar to the well established experimental set up that
is based on the Hanle effect (c.f., for instance, Ref.
\cite{PRB_033305}). Furthermore, the electric field $E_0$ induces
an in-plane spin polarization $f_{+}^{(0)}$.

As in Section 3, the effect of the SAW is treated by a
perturbation expansion $f_z=f_z^{(0)}+\delta f_z$ and
$f_{+}=f_{+}^{(0)}+\delta f_{+}$. The Fourier transformed basic
Eqs.~(\ref{b1}) and (\ref{b2}) are easily solved, when non-linear
perturbations are neglected. The solution for the lowest-order
Fourier components is given in the Appendix.

To determine the steady-state spin polarization under the mutual
influence of a constant electric field and the SAW field, we focus
on the most interesting case $\alpha=\beta$ and assume
$\Omega_E\tau_M\gg 1$. Under these conditions, the solution given
by Eqs.~(\ref{A3}) to (\ref{A5}) simplifies and takes the form
\begin{equation}
\frac{\delta
f_{+}(0)}{f_{+}^{(0)}}=-\frac{Y_{SAW}^2\Omega_E}{2(1+\Lambda_{+}^2)}{\rm
Re}\Biggl\{\frac{\Omega_E(1-q^2)Z_1
+\Omega(1-\Lambda_{+}^2-2iq\Lambda_{+})}{(\Omega-\Omega_{+})(\Omega-\Omega_{-})}
\Biggl\},
\end{equation}
\begin{equation}
\frac{\delta
f_{z}(0)}{f_{z}^{(0)}}=\frac{Y_{SAW}^2\Omega_E}{2\Lambda(1+\Lambda_{+}^2)}{\rm
Re}\Biggl\{\frac{\Omega_E(1-q^2)Z_2
+i\Omega(1-\Lambda_{+}^2+2iq\Lambda)}{(\Omega-\Omega_{+})(\Omega-\Omega_{-})}
\Biggl\},
\end{equation}
with the shorthand notations
$Z_1=3\Lambda_{+}-1+i\Lambda(1-\Lambda_{+}^2)$,
$Z_2=\Lambda(3-2i\Lambda +\Lambda_{+}^2)$, $q=K_{+}/K_{SAW}$, and
$\Lambda_{+}=q\Lambda$. The eigen-frequencies of the spin
excitations are expressed by
\begin{equation}
\Omega_{\pm}=\mu E_0(K_{SAW}\pm K_{+})-iD(K_{SAW}\pm K_{+})^2.
\label{disper}
\end{equation}
The appearance of resonances at $\Omega=\Omega_{\pm}$ that occur
in the in-plane and out-of-plane field-induced spin polarization
is the most remarkable result of this paper. Due to the
spin-rotation symmetry, a soft mode develops in the system that
can be probed by a SAW, which provides the wave vector $K_{SAW}$
for the resonant excitation. The low-frequency mode
$\Omega\rightarrow 0$ becomes increasingly undamped for
$K_{SAW}\rightarrow \pm K_{\pm}$. As a remnant of these coherent
long-lived spin excitations, a weakly damped resonance appears,
when the applied constant electric field $E_0$ satisfies the
condition $\Omega=v_{SAW}K_{SAW}=\mu E_0(K_{SAW}-K_{+})$.

Numerical examples are shown in Figs. \ref{fig1} and \ref{fig2}
for the SAW-induced
\begin{figure}
\begin{minipage}[l]{0.47\textwidth}
\includegraphics[width=2.5in]{fig1}%
\caption{\small SAW-induced stationary in-plane spin polarization
$\delta f_x(0)$ referred to $f_x^{(0)}Y_{SAW}$ for
$\lambda_{SAW}=5.6$ $\mu$m, $\mu=2.3\,10^{4}$ cm$^{2}$/Vs, and
$D=24$ cm$^{2}$/s. Results are shown for $K_{+}/K_{SAW}=$ 0.8,
0.85, and 0.9.} \label{fig1}
\end{minipage}%
\hspace{0.5cm}
\begin{minipage}[r]{0.47\textwidth}
\includegraphics[width=2.5in]{fig2}%
\caption{\small SAW-induced stationary out-of-plane spin
polarization $\delta f_z(0)$ referred to $f_z^{(0)}Y_{SAW}$ for
$\lambda_{SAW}=5.6$ $\mu$m, $\mu=2.3\,10^{4}$ cm$^{2}$/Vs, and
$D=24$ cm$^{2}$/s. Results are shown for $K_{+}/K_{SAW}=$ 0.9 and
0.925.} \label{fig2}
\end{minipage}
\end{figure}
in-plane and out-of-plane spin polarization. The parameters used
in the calculation refer to GaAs quantum
wells.\cite{PRL_036603,PRL_047602} It is to be noted that in the
displayed relative spin polarizations, the electric field $E_0$
enters via the field-dependent quantities $f_x^{(0)}$ and
$f_z^{(0)}$ calculated from Eq.~(\ref{fz0}). Both components of
the magnetization exhibit a sharp resonance in the electric field
dependence at $\mu E_0=v_{SAW}/(1-K_{+}/K_{SAW})$ as indicated by
the vertical line in Fig.~\ref{fig2}. With increasing ratio
$K_{+}/K_{SAW}$, the resonance is shifted to higher field
strengths and becomes more pronounced. Under the condition
$E_{SAW}\approx E_0$ and at the resonance, the out-of-plane spin
polarization may significantly exceed the spin generation
$f_z^{(0)}$ given in Eq.~(\ref{fz0}). As the suppression of
$f_z^{(0)}$ at high electric fields can be compensated by an
appropriate in-plane magnetic field~\cite{PRB_075340}, the
experimental demonstration of the effect should be feasible. Its
most salient feature is the strong variation of the field-induced
magnetization in the vicinity of the resonance field strength.
This switching of the magnetization caused by an applied constant
electric field could be useful for future spintronic device
applications.

\section{Summary}
Recently, long-range transport of spins has been experimentally
demonstrated in [001] GaAs quantum wells with balanced Rashba and
Dresselhaus terms as well as in Dresselhaus [110] quantum wells.
The idealized model that describes both systems exhibits an exact
spin rotation symmetry with an associated soft mode and a
persistent spin helix. This long-lived spin coherence state is
transferred to a field-dependent eigenmode of the system, when a
constant in-plane electric field is applied. To resonantly probe
the field-induced excitation, the required wave-vector must be
provided by an appropriate experimental set up. Similar to the
well established physics of space-charge waves one can produce
optical gratings for that purpose. In this paper, we treated an
excitation mechanism via an acoustic wave propagating along a
[001] GaAs quantum well, in which both Rashba and Dresselhaus SOI
exist. Due to the spin-charge coupling, specific eigenmodes are
identified both in the charge current density and the in-plane and
out-of-plane spin polarizations. The SAW-induced change of the
stationary charge current is composed of two contributions. The
first one is independent of the SOI and exhibits a pole that is
due to oscillations of the free carrier density. In the second
contribution, which is related to the field-induced homogeneous
spin accumulation, a new eigenmode appears with the dispersion
relation $\Omega=\mu E_0 K_{SAW}- (DK_{SAW}^2+2/\tau_{s-})$. In
this equation, the spin-scattering time $\tau_{s-}$ (which
diverges in the case $\alpha=\beta$) takes over the role of the
Maxwellian relaxation time $\tau_M$ that is responsible for the
damping of pure charge oscillations.

Characteristic field-dependent eigenmodes appear also in the
SAW-induced components of the magnetization. Most interesting is
the case, when the Rashba and Dresselhaus coupling strengths
become equal. According to the dispersion relation
$\Omega=\Omega_{-}$, a undamped soft mode occurs, when the
wave-vector $K_{SAW}$ of the SAW approaches the shifting vector
$K_{+}=2m(\alpha+\beta)/\hbar^2$. As a remnant of this persistent
spin helix, a sharp resonance occurs in the electric-field
dependence of the in-plane and out-of-plane magnetization at $\mu
E_0=v_{SAW}/(1-K_{+}/K_{SAW})$. In the vicinity of this resonance,
the spin polarization drastically changes with a slight variation
of the electric field strength. It is a challenge to
experimentally verify this field-induced switching of
magnetization in a 2DEG with balanced Rashba and Dresselhaus SOI.

redpajama_set_name: RedPajamaArXiv


text:
Cole On Not Being BFF With Drake, Groupies vs. Girlfriend And Lebron James (Pg. 2)
May 18, 2010 - 6:45 pm by Tray Hova
About a month ago, Drake mentioned the possibility of you jumping on a Thank Me Later bonus cut. Fact?
Man, me and Drake have been trying to get something done. Actually, if he reads this, tell him to send the shit he supposed to send. [Laughs] I understand we both busy and we spoke about doing some shit, but I guess schedule wise it hasn't worked out. That would be ill, but as of now it's not done.
What's an actual conversation like between you guys? Is it past a 'What's good' and 'Congrats'?
It's not that type of relationship yet. Right now, it's a mutual respect, like I see what you're doing, you're killing the game, I'm a fan or whatever the case is. We're both young and even though he's more established and has hits, he still doesn't have an album out. He still has to prep for that. So we're not in the position to be best friends. We can save that for when we're both laid up and chilling, but right now we both have work to do. There's not many rappers who I feel I really know. I think Wale is one of the few that I have a real friendship with. Not saying that won't happen with Drake because you never know, but right now it starts with respect.
No other industry friends you confide in?
Nah man. Even Wale… I don't want to get that twisted like we have deep conversations about life. I just feel like I know him better than the others. I keep to myself by nature.
I bet the groupies don't like that. How are you handling them?
[Laughs] I haven't figured it out, but it's not like that for me. I can't tell you crazy groupie tales. I mean they scream and go crazy as if I'm Drake. [Laughs] The craziest thing that's happened so far is girls just asking me to sign their breasts, but there hasn't been any wild backstage stories. I truly believe that your mentality attracts certain things. It's almost like [groupies] can feel the energy I give off, like it's probably not going to go down. I mean, I notice them, but that energy stops them in their tracks. That must be what's happening.
"Nas actually quoted one of my lines. I was like 'Man, don't quote me'... I used to type Nas lyrics just to put up on my wall"
Safe to assume you're still with your girlfriend?
[Laughs] Yes, we're still together.
It's easy to count blessings right now, but what do you think has been your biggest mistake thus far?
Hmm, I don't feel like I have any big mistakes. I have missteps, but those all led me to something greater. It wasn't a harsh lesson, but I learned to be careful with who you let onto your team. Because these people at the end of the day are going to reflect you. If you've got a bunch of assholes around you, people might look at you in that light. I don't want to go into specifics, but I learned that early.
On a lighter note, who are some well-known folks you were surprised to learn are J. Cole fans?
LeBron! I met LeBron at a show in Cleveland and his homeboy tells me, 'Yo I 'm loving the mixtape, especially that one joint, that turn off the lights joint.' Then LeBron jumps in the conversation—mind you I hadn't even spoken to him and this nigga got a deep-ass voice—singing "Lights Please." I was like 'What you know about that? Please don't tell me LeBron James listens to my mixtape!'
What was your reaction to the Nas cosign?
LeBron James,
Beyoncè's Ivy Park x Adidas Collaboration Is Already A Major Success
The internet has been buzzing with anticipation for Beyonce's new Ivy Park x Adidas collaboration so its no surprise that the line sold out in a day. Pre-sale items from the new collection, and Bey's first with Adidas after dropping Top Shop and becoming the sole owner, went on sale on Friday (Jan. 17). By the end of the day, the only items still available were Ivy Park socks and even those were sold out by Saturday.
The line consists of an orange burgundy and off-white color pallet and includes track pants, jackets, hoodies, dresses, sneakers, bras, bodysuits, cycling shorts, fanny packs, and more.
Live on https://t.co/SDScvRTZ6p 12 PM PST pic.twitter.com/ozhQd1chIx
— BEYONCÉ (@Beyonce) January 17, 2020
Beyoncé for adidas x IVY PARK.#adidasxIVYPARK pic.twitter.com/jnBa6OEfCI
— BEYONCÉ LEGION (@BeyLegion) January 17, 2020
"My team has worked hard with the adidas team in bringing my vision to life for the first collection and I am grateful and proud," Bey said in a statement last year. "From the accessories to the clothes and footwear, I wanted to design and re-imagine pieces that serve as favorite armor for anyone who acknowledges the strength in their individual style and lives freely and boldly."
Prior to the launch, Bey gifted some of her celebrity friends and family members including her mother, Tina Lawson, Kelly Rowland, Yara Shihidi, Janelle Monae, Ciara, and stylist June Ambrose, with the entire Ivy Park x Adidas collection.
Portions of the collection are still available at select Adidas stores, as well as Nordstorm, Bloomingdale's, ASOSA, Finish Line and Foot Locker.
In other Yonce news, the "Spirit" singer reportedly signed a new publishing deal with SONY/ATV.
Nipsey Hussle attends the 61st Annual GRAMMY Awards at Staples Center on February 10, 2019 in Los Angeles, California.
Nipsey Hussle Rumored To Receive Tribute At 62nd Annual Grammy Awards
This time last year, Nipsey Hussle attended the Grammy Awards as a first-time nominee. The Los Angeles native, who earned a nod for his long-awaited feature length studio album, Victory Lap, hit the red carpet alongside his daughter, Imani, and partner Lauryn London. Despite losing the category to Cardi B, Hussle's landing a nomination after years of grinding in the rap game, was a victory within itself.
"It ain't expect nothing," he told Big Boy's Neighborhood last last year of being nominated.. "It's been some talk around it so if the list would've come around and I wasn't on it, I wasn't going to be disappointed."
Two months after the award show, the 33-year-old rapper and entrepreneur was gunned down in the parking lot of his clothing store. Hussle's tragic death seemingly expanded his fans based an illuminated his legacy and influence, and according to a report from Hits Daily Double, the Grammys will pay tribute to the late recording artist during this year's ceremony. It's unclear who will participate in the supposed tribute as the Recording Academy has yet to confirm (or deny) the rumor.
Hussle also received three posthumous Grammy nods for Best Rap Song, Best Rap Performance and Best Rap/Sung performance. The ceremony is expected to feature performances from Tyler the Creator, H.E.R., Charlie Wilson, Lil Nas X, BTS, Lizzo, and Aerosmith with Run DMC, and more.
The 62nd annual Grammy Awards air on Jan. 26 on CBS.

redpajama_set_name: RedPajamaCommonCrawl


(25) Logical failure: Shakespeare was Shakespeare !
Shakespeare's comprehensive education requires, for example, that he must have visited the school in Stratford. But there is no evidence that the person from Stratford Shakspere has ever attended school, nor that he could ever write fluently. A question , put to the test, is from the outset accepted, because "a necessary precondition".
With Shakespeare, this question seems to be resolved. Nobody would ask : "Which Shakespeare?"


text:
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redpajama_set_name: RedPajamaGithub


2 In terms of market share, ChannelAdvisor is clearly lagging behind, losing to Unica in all segments.
1 Unica has better usage coverage in more websites categories. Including Business & Industry, Autos & Vehicles, Health, Arts & Entertainment and 17 other categories.
2 ChannelAdvisor is leading in Shopping, Food & Drink, Beauty & Fitness and Books & Literature.
1 Unica is leading in most countries, including United States, Japan, United Kingdom, Canada and 72 other countries.
2 ChannelAdvisor is leading in Ukraine, Philippines, Vietnam, Saudi Arabia and 3 other countries.


We are a talented team where each member brings unique talents and experience. Our passion is to help companies of all sizes build their image, brand and ultimately sales.
B&W Wholesale provides you with all you need to promote your business, hats and apparel both screenprinted and embroided, bags, pens, table covers, office supplies, trade show items, all with your logo, and great customer service.
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Its all about colors! I always love the combination of blue and green hues, being nature colors it creates a soothing and relaxing mood. But when these pastels are used vibrantly it instantly stands out from the background energetic and lively. Most importantly its attractive and appealing to the eyes. Just wanted to get out of the periodic pastels and embellish with a vibrant decor for a Baby Shower... Yes, this color scheme sets the theme for the setoff to host for my best buddy!
The centerpiece was Onesies Cupcakes that I throughly enjoyed. Don't you think these cute little decorative cupcakes are a perfect gift giving? Some of them thought these cupcakes were edible. Surprisingly these two hues played together very well not only for baby shower, but also for a birthday party.
Love the color combo...always loved it....you are creative and especially when coming to colors....to be in a party with these decorations will be sure one of the best moments in life...love the idea of stacked up balloons.. it looks awesome among all these great decor...great work.
It is an amazing Horse/ Pony Themed Party Décor. The colors are so amazing. From the cakes and food I loved everything else. Keep sharing the photos here. I too have been making use of the fabulous spider man theme for my son's birthday. It is going to be so fun but I am not sure about the affordable Chicago venues. I wonder if you could help regarding it.


Have a look at the manual Acura Embedded AcuraVision Camera Detect Events guide online for free. It's possible to download the document as PDF or print. UserManuals.tech offer 51 Acura Embedded manuals and user's guides for free. Share the user manual or guide on Facebook, Twitter or Google+.
7. Use free hand sketching to wipe out Mask areas.
you to a precise detection area.
event such as Motion event, select it from the Type list.
camera, select the camera number from the Camera list.
messages(include Flow Counting messages) will be found.
subject, type your text in the provided text box.
Sender             Specify the senders e-mail address.
add the e-mail address to the Address list.
Modify          Modify an e-mail address.
Test             To test sending an email.
detected event as email attachment.
Size                             Set the image dimensions.
Number                       Attachment can be up to 6 images.
from 1 to 5 seconds.
sound the alarm until the event terminates.
corner of a split screen on Site Server when an event is detected.