"Dad has visions of her sitting in the rocking chair with a shawl around her and a dickey around her neck. She was a very stately person. One of the last things before she passed away she had Flora get her a new dickey that she wanted to be buried in.
"She died of old age.
"My grandmother would go out to the farm where her daughter, Minnie, lived, and Flora would be coming home from school. Grandma Lowell would go out there to clean the house up from dirt and cats. One time, Grandma was chasing them out the back door and the hired man Jones was shooting them. Granma was the matriarch and called the shots.
1900 Census, listed with John Lowell in Wall Lake Township, Minnehaha Cty, South Dakota.
Sioux Falls SD City Directory 1909 lists Lowell, Viola (wid John) r.1024 W. 9th.
Flora G., granddaughter, 19, single, born in SD, father's birthplace listed as un, mother born in WI.
"Miss Flora McCartney of this city, who, with her grandmother, Mrs. John Lowell, are spending the summer in the east, has entered Columbia university where she is doing some advanced work."
1930 Census: is listed as living with her granddaughter, Flora Luker, in Gainesville. See Luker entry for census information.
At the John R. Lowell home, North Lincoln avenue, a group of elderly women gathered Friday to help Mrs. Viola Lowell celebrate her 85th birthday.
The afternoon was passed recalling reminiscences by the many who had lived here in pioneer days.
In the dining room where refreshments were served a beautiful pyramid cake was the centerpiece and was lighted with 15 candles.
After serving the table was cleared and Grandma Lowell was presented with many gifts and greetings which she opened and read, also acknowledging the gifts as they were passed to her by the donors."
Death certificate lists age at time of death as 89 years, 8 months, and 23 days and name of father as Abraham Furdesh born in Canada and name of mother as Nancy Peterson born in Maine.
Mrs. Viola Lowell, 89 years old, 1201 North Lincoln Ave., West Sioux Falls, died today at her home as a result of complications resulting from the infirmities of age. Mrs. Lowell had been a resident of this vicinity for 49 years and was the widow of John F. Lowell.
She was born, February 8, 1844 in Maine, and came to this section of the country when she was 40 years old. The body is at the Miller Funeral home pending the completion of plans for final rites. Present arrangements include the services of Dr. John F. Robertson, pastor of the First Methodist Episcopal Church, as the officiating clergyman, with interment in Woodlawn Cemetery.
Surviving are a daughter, Mrs. Minnie L. McArtney, Tea, a son, John R. Lowell, West Sioux Falls; a brother, Frank L. Furdesh, Massachusetts; four grandchildren, and two great grandchildren."
Funeral services for Mrs. Viola Lowell, 89 years old, a resident of this vicinity for nearly 50 years, will be held at 2.30 o'clock Friday afternoon at the Miller chapel. Rev. John F. Robertson, pastor of the First Methodist Episcopal church, will officiate.
The funeral hymns will be sung by Norman Mathers, accompanied by Mrs. C.B. Van Ausdall at the pipe organ. The pallbearers will be A. Erskine, Grant Bartram, S. Munson, S. Smith, Edward Shotwell, and Matt Krell. Interment will be in Woodlawn Cemetery, beside the grave of her husband, who preceded her in death 25 years ago.
Mrs. Lowell died Tuesday morning at 4.15 o'clock after an illness of six weeks, at the home of her son, J.R. Lowell, 1201 North Lincoln ave.
She was born February 8, 1844, at Rockland, Maine, the daughter of Abraham and Nancy Furbish, the fourth of a family of seven children. In 1863 she married John P. Lowell [sic], at Farmington, Maine, and immediately thereafter the couple took up their residence in Wisconsin, where Mr. Lowell was engaged in the lumbering business.
In 1884 the family moved to this vicinity and lived for 15 years on a farm situated 12 miles west of the city. Then the Lowells took up their residence in Sioux Falls. In the latter part of her life, Mrs. Lowell spent considerable time in the milder climates of California and Florida, as well as various other parts of the United States.
She is survived by a son, John R. Lowell of North Lincoln avenue, and a daughter, Mrs. M. L. McCartney of near Tea; four grandchildren, Mrs. Flora G. Luker, George, John, and Charles Lowell; two great-grandchildren, Jimmie and John Lowell, all of this vicinity, and a brother, Frank Furbish, Graniteville, Mass."
Funeral services for Mrs. Viola Lowell, 89 years old, a resident of this vicinity for nearly 50 years, were held this afternoon at Miller chapel. Mrs. Lowell died Tuesday morning after an illness of six weeks, at the home of her son, J. R. Lowell, 1201 North Lincoln ave.


text:
\subsection{$M\mathcal{T}$ symmetry and its spontaneous breaking}\label{AA}
The low-energy effective Hamiltonian is introduced in Eq. (1) of the main text. Here we describe a symmetry that relates the two valleys under consideration.

We are interested in the (001) surface of TCI. It is known from earlier studies that there is a structural distortion occurring spontaneously at low temperature and breaks all rotation symmetry \cite{supp01}. This distortion can happen along either $[110]$ or $[1\bar{1}0]$ direction, and leads to a ferroelectric polarization. Note that this is \textit{not} the quantum Hall ferroelectricity that we study in this paper. Without loss of generality, let us assume the distortion is along $[110]$ and set up the coordinates such that it is the $x$-direction. Because of the ferroelectric distortion, the (001) surface has only the mirror symmetry $M_y$, which reverses the $y$-direction, and time-reversal $\mathcal{T}$. An illustration of the surface Brillouin zone is shown in Fig. \ref{BZ}. The low-energy effective model consists of four Dirac cones, with a massive degenerate pair near $\bar{X}_1$ and a massless degenerate pair near $\bar{X}_2$ \cite{supp13}. The $2+2$-fold degeneracy is protected by $\mathcal{T}$.

\begin{figure}[H]
\centering
\includegraphics[width=0.25\textwidth, height=4.3cm]{BZ.png}
\caption{Surface Brillouin zone of the (001) surface of TCI. There is a pair of Dirac cones near $\bar{X}_1$ and a pair near $\bar{X}_2$. The blue arrow indicates the ferroelectric distortion. }
\label{BZ}
\end{figure}

In the presence of magnetic field, the mirror symmetry $M_y$ and the time-reversal $\mathcal{T}$ are \textit{individually} broken. Still, the product $M_y \mathcal{T}$ remains a symmetry. Notice that $M_y \mathcal{T}$ relates the individual valleys near $\bar{X}_1$ to themselves, while it exchanges opposite valleys near $\bar{X}_2$. Hence, under a magnetic field, such $2+2$-fold degeneracy of Landau levels is explicitly broken down to just the $2$-fold degeneracy for the massless Dirac cones near $\bar{X}_2$. Moreover, such originally massless Dirac cones can now acquire a Zeeman gap, as we explain below.

Let us label the location of the Dirac cones as $\pm \Lambda$. At $+\Lambda$, a two-band model has been constructed before and admits the following form \cite{supp13, supp12}:
\begin{equation}
H_{+\Lambda} = v_x \sigma_y p_x +v_y \sigma_x p_y +\delta v_x p_x +\Delta \sigma_z,
\end{equation}
Here $\delta v_x$ characterizes the tilt of Dirac cone, which is symmetry-allowed and has been observed experimentally \cite{supp15}. The mirror symmetry $M_y$ acts on the pseudo-spin and momentum as follows:
\begin{equation}
M_y : p_x \rightarrow p_x,\; p_y \rightarrow -p_y,\; \sigma_x \rightarrow -\sigma_x,\; \sigma_y \rightarrow \sigma_y, \; \sigma_z \rightarrow-\sigma_z,
\end{equation}
while time-reversal $\mathcal{T}$ acts as follows:
\begin{equation}
\mathcal{T}: p_x \rightarrow -p_x,\; p_y \rightarrow -p_y,\; \sigma_x \rightarrow -\sigma_x,\; \sigma_y \rightarrow -\sigma_y, \; \sigma_z \rightarrow-\sigma_z.
\end{equation}
From these we see that the mass term $\Delta=0$ in the absence of background field, as $M_y$ is a symmetry that relates the cone at $+\Lambda$ to itself but sends $\Delta\sigma_z$ to $-\Delta\sigma_z$. However, in the presence of a magnetic field, $M_y$ is no longer a symmetry, and hence the massless Dirac cone at $+\Lambda$ can acquire mass in general (\textit{i.e.} Zeeman effect). The remaining symmetry is the $M_y \mathcal{T}$ symmetry which relates the cone at $+\Lambda$ to the one at $-\Lambda$:
\begin{equation}
H_{-\Lambda} = (M_y \mathcal{T})H_{+\Lambda}(M_y \mathcal{T})^{-1}= v_x \sigma_y p_x +v_y \sigma_x p_y -\delta v_x p_x +\Delta \sigma_z.
\end{equation}
To simplify notation, we rotate the basis: $\sigma_x \rightarrow -\sigma_y,\; \sigma_y\rightarrow \sigma_x, \; \sigma_z \rightarrow \sigma_z$ and obtain the following unitarily equivalent Hamiltonian:
\begin{equation}\label{LambdaHam}
H_{\pm \Lambda} = v_x \sigma_x p_x -v_y \sigma_y p_y \pm \delta v_x p_x +\Delta \sigma_z.
\end{equation}
This is Eq. (1) in the main text, which provides the starting point for our study. In the main text, we have referred to the symmetry that protects the degeneracy of the two valleys as a ``two-fold rotation" or ``inversion" symmetry, but when applied specifically to the surface of TCI, it has a precise meaning as the $M\mathcal{T}$ symmetry. This symmetry is spontaneously broken by Coulomb interaction and results in a valley-polarized state.

\subsection{Massive and tilted Dirac Landau levels}\label{A}
\setcounter{equation}{0}
Assuming valley-polarization, we focus on the one at $+\Lambda$. Under an out-of-plane magnetic field $-B\hat{z}$, in the un-tilted limit, the massive Dirac Hamiltonian in Eq. (\ref{LambdaHam}) can be written as
\begin{equation}
H_0=\frac{\sqrt{2}\;v}{l_B} \begin{pmatrix}
\lambda & a^\dagger \\
a & -\lambda
\end{pmatrix}
\label{dirac}
\end{equation}
where $ v=\sqrt{v_x v_y}$, magnetic length $l_B=\sqrt{\hbar c/eB}$  and the mass parameter $\lambda = \Delta l_B/(\sqrt{2}v)$. Here, $a^\dagger, a$ are parabolic Landau level raising and lowering operators respectively, and are related to the momentum operators by:
\begin{equation}\label{rescaledmomentum}
\begin{split}
p_x= \frac{1}{l_B}\sqrt{\frac{v_y}{2v_x}} (a^\dagger +&a)\;,\quad p_y =\frac{i}{l_B}\sqrt{\frac{v_x}{2v_y}}(a-a^\dagger)\\ &[a,a^\dagger]=1
\end{split}
\end{equation}

The wavefunctions of the massive Dirac Landau levels and their corresponding energy can then be solved exactly. For the $n$-th Landau level with $n \neq 0$:
\begin{equation}
\begin{split}
&\psi_{n,m} = \frac{1}{\sqrt{1+\gamma_{n}^2}} \begin{pmatrix}
\phi_{\abs{n},m} \\ \gamma_{n} \phi_{\abs{n}-1,m}
\end{pmatrix},\quad E_{n} = s_n \frac{\sqrt{2}\;v}{l_B}\sqrt{\lambda^2 +\abs{n}}
\end{split}
\end{equation}
where
\begin{equation}
\gamma_{n}=\frac{-\lambda +s_n \sqrt{\lambda^2 +\abs{n}\;}}{\sqrt{\abs{n}}}
\end{equation}
Here $s_n=\text{sgn}(n)$, and $\phi_{\abs{n},m}$ are the wavefunctions for a parabolic Landau level in the symmetric gauge with angular momentum $m-\abs{n}$. For the 0-th Dirac Landau level, we have:
\begin{equation}
\psi_{0,m} = \begin{pmatrix}
\phi_{0,m} \\0
\end{pmatrix}, \quad\; E_0 = \frac{\sqrt{2}\;v}{l_B}\lambda
\end{equation}

When the tilt of Dirac cone $\delta v_x$ is turned on, we can do first order perturbation theory to obtain the approximate eigenstates. To leading order in $\tau = \delta v_x / (2v_x)$, for the $n\neq 0$ massive and tilted Dirac LL, we obtain (up to normalization):
\begin{equation}\label{tiltedDirac}
\psi_{n,m} =
\begin{pmatrix}
\phi_{\abs{n},m} \pm \tau [\alpha_{-1}\phi_{\abs{n}-1,m} +\alpha_1\phi_{\abs{n}+1,m}] \\
\gamma_{n} [\phi_{\abs{n}-1,m} \mp \tau(\alpha_0 \phi_{\abs{n},m} +\alpha_{-2}\phi_{\abs{n}-2,m} )]
\end{pmatrix}
\end{equation}
\noindent where
\begin{equation}\label{alpha}
\small{\begin{split}
&\alpha_{-1} = \frac{(2\abs{n}-1)\sqrt{\lambda^2+\abs{n}} \pm \lambda}{\sqrt{\abs{n}}}\;,\;\alpha_1= - 2\sqrt{\abs{n}+1}\sqrt{\lambda^2+\abs{n}}\\
&\alpha_0 = \frac{(2\abs{n}+1)\sqrt{\lambda^2+\abs{n}} \pm \lambda}{\sqrt{\abs{n}}}\;,\;\alpha_{-2}= - 2\sqrt{\abs{n}-1}\sqrt{\lambda^2+\abs{n}}
\end{split}}
\end{equation}
As for the massive and tilted $0$-th Dirac LL:
\begin{equation}
\psi_{0,m} = \begin{pmatrix}
\phi_{0,m}-2\tau \lambda \phi_{1,m} \\ -\tau \phi_{0,m}
\end{pmatrix}
\end{equation}
These expressions allow us to calculate dipole moments, and energy shifts under the influence of impurity, straightforwardly.

\subsection{Number of impurity states for massive and tilted Dirac cones}\label{B}
\setcounter{equation}{0}
Here we demonstrate that there are only two states that have probability amplitudes at the impurity site, and which therefore are split from the Landau level, even in the presence of perturbations in mass and tilt of the Dirac cone.

We consider a delta-function impurity $H_{imp}=V_0 l_B^2 \delta(\vec{x})$. Upon projection to a specific Landau level, the impurity Hamiltonian has matrix elements:
\begin{equation}
\bra{n,m}H_{imp}\ket{n,m'} = V_0 l_B^2 \Psi^\dagger_{n,m}\Psi_{n,m'}
\end{equation}
where we have defined $\Psi_{n,m} \equiv \psi_{n,m} (\vec{0})$, $i.e.$ the amplitude of the Landau level orbital at the impurity site. To the first order in tilt $\tau$, the Dirac Landau level is found in Eq. (\ref{tiltedDirac}). To prove our claim in full generality, let us assume we have carried out a $k$-th order perturbation theory in $\tau$, so that the $n$-th tilted Dirac Landau level $\psi_{n,m}$ is expressed in terms of $\phi_{p,m}$ with $p=\abs{n}-k-1,...,\abs{n}+k$. The only states that are relevant to our impurity problem are those that have non-vanishing probability amplitudes at the impurity site, which correspond to those $\psi_{n,m}$ with $m=\abs{n}-k-1,...,\abs{n}+k$. We thus study the degenerate perturbation theory within this subspace, and consider linear combinations of $\Psi_{n,m}$:
\begin{equation}\label{eq19}
\Phi=r_1\Psi_{n,\abs{n}-k-1}+r_2\Psi_{n,\abs{n}-k}+...+r_{2k+2}\Psi_{n,\abs{n}+k}
\end{equation}
If there is a choice of $(r_1,r_2,...,r_{2k+2})$ such that $\Phi = (0,0)^T$, the corresponding linear combination of intra-Landau level orbitals are guaranteed to diagonalize the impurity Hamiltonian and thus remain at the same energy as the Landau level in the absence of impurity. Below, we argue that there are $2k$ such solutions.

Denote $\Psi_{n,m} = (\psi_{m}^\uparrow,\; \psi_{m}^\downarrow)^T$. Only the intra-Landau level index $m$ is made explicit here. Notice that $\psi_{m}^\uparrow$ and $\psi_{m}^\downarrow$ are both real or both imaginary. This is because each of them is proportional to the wavefunction of parabolic Landau level $\phi_{m,m}$ evaluated at the origin, which is real when $m$ is even and is imaginary when $m$ is odd. Redefining $i\Psi_{n,m} \mapsto \Psi_{n,m}$ for odd $m$, Eq. (\ref{eq19}) with $\Phi=(0,0)^T$ becomes a set of simultaneous equations for \textit{real} unknowns $r_i$. Setting $r_{2k+2} =1$ without loss of generality, we reach the following set of equations for $r_i \in \mathbb{R}$:
\begin{equation}\label{eq20}
\begin{cases}
\small{r_1 \psi^{\uparrow}_{n-k-1} + r_2 \psi^{\uparrow}_{n-k}+ ... + r_{2k+1} \psi^{\uparrow}_{n+k-1} = -\psi^{\uparrow}_{n+k}} \\
\small{r_1 \psi^{\downarrow}_{n-k-1} + r_2 \psi^{\downarrow}_{n-k}+ ... +r_{2k+1} \psi^{\downarrow}_{n+k-1} = -\psi^{\downarrow}_{n+k}}
\end{cases}
\end{equation}

With $2k+1$ unknowns and only two linear equations, there are in general $2k$ linearly independent solutions, leading to $2k$ states that have vanishing amplitudes at the impurity site. Since we start with a $(2k+2)$-dimensional subspace, only $2k+2-2k=2$ states are allowed to have non-vanishing amplitudes at the origin. These are the two impurity bound states whose energy are split from the bulk Landau level, and are the ones employed in our construction of impurity dipole moment in the main text.

The above argument also works for the 0-th Landau level. However, only one impurity state is significantly shifted away from the bulk Landau level, while the shift of the second impurity state is minuscule (controlled by the size of the tilt), so practically, in the quantum Hall ferroelectric system that we consider, only one impurity state can be probed in this special case.

\subsection{Choice of Parameters}\label{C}
In the main text, we use the following parameters to study the quantum Hall ferroelectrics in topological crystalline insulator Sn$_{1-x}$Pb$_x$(Te,Se):
\begin{equation}\label{C1}
\tau=0.1,\quad \lambda=0 ,\quad v_x/v_y=1.6
\end{equation}
Here we explain why these values match with the low-energy physics of the system obtained either from experiments or \textit{ab initio} calculations.

The tilting effect of Dirac cones (at $\bar{\Lambda}$) has been observed in the ARPES measurements by Tanaka \textit{et al.} \cite{supp15}, from which we estimate the tilting parameter to be $\tau=\delta v_x/(2v_x)=0.1$. The acquisition of mass in topological crystalline insulators was observed by Okada \textit{et al.} \cite{supp5}. Under a ferroelectric distortion, two of the four surface Dirac cones were measured to obtain mass of about $\Delta=10 $ meV, and this would correspond to $\lambda=\Delta l_B/(\sqrt{2}v)\approx 0.5$. But notice that these two massive cones are located near $\bar{X}_1$ (see Fig. \ref{BZ}), which are not symmetry-related in our quantum Hall setting. In our study we are instead focusing on the Dirac cones near $\bar{X}_2$, whose degeneracy is symmetry-protected as explained in Sec. \ref{AA}. These cones can acquire a mass via the Zeeman effect, but the experiment by Okada \textit{et al.} \cite{supp5} suggests that it is too small to be observed. A rough estimate with the vacuum Zeeman effect would give $\lambda \sim 0.01$, and thus in the main text we decide to assume $\lambda=0$. The values of $v_x$ and $v_y$ have been obtained by Liu \textit{et al.} by fitting with \textit{ab initio} calculations \cite{supp12}. For the effective Dirac Hamiltonian (around $\bar{\Lambda}$) that we are considering, $v_x=1.3$ eV$\AA$ and $v_y=0.83$ eV$\AA$. Thus, the anisotropy $v_x/v_y=1.6$.

\subsection{Relation between the local impurity dipole and the bulk adiabatic dipole}\label{CD}
Here we present more details of the derivations of Eqs.(4) and (6) in the main text. \\

Let us begin with the bulk adiabatic dipole moment introduced in the modern theory of polarization \cite{supp1}. Since the tilt of Dirac cone in our model breaks inversion symmetry in the $p_x$-direction, electric polarization is non-vanishing only in the $y$-direction and we thus focus only on that component. Following the conventional Berry phase approach, we have \cite{supp2}:
\begin{equation}\label{CD1}
D_y = ie\frac{l^2_B}{L_x}\int_{0}^{L_x/l^2_B}dk_y\;\bra{u_{k_y}}\partial_{k_y}\ket{u_{k_y}}
\end{equation}
where $\ket{u_{k_y}}$ is the Bloch wavefunction in a gauge which is invariant under translation in $y$-direction. In this gauge, the complete wavefunction is $\psi_{k_y}(x,y) = \frac{e^{ik_y y}}{\sqrt{L_y}}u_{k_y}(x)$. Making use of $u_{k_y}(x) = u_0(x-k_y \_B^2)$, one can recast Eq.(\ref{CD1}) into the following form:
\begin{equation}
\begin{split}
D_y&=-i e l^2_B \int d^2 r\;\psi^*_{k_y}(x,y) \partial_x \psi_{k_y}(x,y) \\
&= e l^2_B \bra{\psi_{k_y}}p_x\ket{\psi_{k_y}}
\end{split}
\end{equation}
Expressing the momentum operator in terms of inter-Landau level ladder operators as in Eq. (\ref{rescaledmomentum}), and acting it on the first-order perturbed Landau orbitals in Eq. (\ref{tiltedDirac}), one would obtain Eq. (4) of the main text:
\begin{equation}\label{CD2}
\begin{split}
&{\bf D}_{n} =  {\tilde s}_{n} \sqrt{2}\;\tau\; e \;l_B\;\left(\frac{2\lambda^2+3|n|}{\sqrt{\lambda^2+|n|}}\right)\sqrt{\frac{v_y}{v_x}} \hat{{\bf y}},
\end{split}
\end{equation}
where $\tilde{s}_n = \text{sgn}(n)$ (and $\tilde{s}_0=1$).
\\

Next we turn to the local impurity dipole moment, which is defined as
\begin{equation}\label{CD3}
{D}^{\rm imp}_y= e(\bra{\tilde{\psi}_1}\hat{y}\ket{\tilde{\psi}_1}+ \bra{\tilde{\psi}_2}\hat{y}\ket{\tilde{\psi}_2}),
\end{equation}
where $\tilde{\psi}_{1,2}$ are the two impurity states bound to the delta-potential defect. Expressing the position operator $\hat{y}$ in terms of the guiding-center operator and the momentum operator: $\hat{y}=\hat{R}_y-l^2_B \hat{p}_x$, it follows that:
\begin{equation}\label{CD4}
D^{\rm imp}_y = e(\bra{\tilde{\psi}_1}\hat{R}_y\ket{\tilde{\psi}_1}+\bra{\tilde{\psi}_2}\hat{R}_y\ket{\tilde{\psi}_2}) - 2D_y.
\end{equation}
Notice that the guiding-center operator can be expressed in terms of \textit{intra}-Landau level ladder operators: $\hat{R}_y = il_B(b^\dagger-b)/\sqrt{2} $. To proceed analytically, we first consider the massless limit and to leading order in the tilt of Dirac cone. The impurity states for the $n$-th Landau level have the following expressions:
\begin{subequations}\label{CD5}
\begin{align}
\tilde{\psi}_1&=-s_n\frac{i\tau\alpha_{-2}}{\sqrt{2}}\psi_{n,n-2}+(-\frac{1}{\sqrt{2}}+\frac{\tau n}{\sqrt{2}})\psi_{n,n-1}+s_ni(\frac{1}{\sqrt{2}}+\frac{\tau n}{\sqrt{2}})\psi_{n,n}-\frac{\tau\alpha_1}{\sqrt{2}} \psi_{n,n+1}\\
\tilde{\psi}_2&=s_n\frac{i\tau\alpha_{-2}}{\sqrt{2}}\psi_{n,n-2}+(\frac{1}{\sqrt{2}}+\frac{\tau n}{\sqrt{2}})\psi_{n,n-1}+s_ni(\frac{1}{\sqrt{2}}-\frac{\tau n}{\sqrt{2}})\psi_{n,n}-\frac{\tau\alpha_1}{\sqrt{2}} \psi_{n,n+1}
\end{align}
\end{subequations}
where $s_n = \text{sgn}(n)$. Note that $\psi_{n,m}$ and $\alpha_i$ are defined in Eqs. (\ref{tiltedDirac}) and (\ref{alpha}) respectively. Combining Eqs. (\ref{CD4}) and (\ref{CD5}), we obtain:
\begin{equation}\label{CD6}
{\bf D}_{n}^{\rm imp} = \frac{2}{3} {\bf D}_{n}
\end{equation}
in the massless limit. For the massive case, the algebra becomes complicated without specifying an explicit LL index. For $n=1$ and $n=2$, we have obtained explicit analytic expressions for the impurity states and evaluated the impurity dipole. The result suggests that
\begin{equation}\label{CD7}
{\bf D}_{n}^{\rm imp} = \frac{2|n|}{3|n|+2\lambda^2} {\bf D}_{n}.
\end{equation}
The validity of this expression is further checked numerically for higher Landau levels (see Fig. \ref{impuritydipole}). It is also worth pointing out that for higher Landau levels, we are usually in the regime where $\lambda\ll \sqrt{\abs{n}}$, so the relation in Eq. (\ref{CD6}) for the massless limit is a good approximation.

\begin{figure}[H]
\centering
\includegraphics[width=1\textwidth, height=4.3cm]{impuritydipole.png}
\caption{Numerical checks of the relation between impurity dipole and bulk adiabatic dipole. (a) Impurity dipole $D^{\rm imp}_y$ (with $e$ set to 1) as a function of tilt $\tau$, for the first Dirac Landau level in the valence band with various mass $\lambda$. The dashed line is given by the analytic result in Eq. (\ref{CD6}). (b) and (c): $D^{\rm}_y/\tau$ as a function of tilt $\tau$ for the second and third Landau levels in the valence band respectively. Solid lines represent results from solving the impurity states numerically, while dashed lines are generated using the analytic formula in Eq. (\ref{CD7}). For small enough tilt such that the first-order perturbation theory is sufficient, it is shown that the analytic result complies with the numerical calculation. Note that the figures here show the analysis for Landau levels in the valence band ($n<0$), which differ from the situation in the conduction band ($n>0$) simply by a minus sign in the dipole.}
\label{impuritydipole}
\end{figure}

\subsection{Differences in the two notions of electric dipole moment}\label{D}
\setcounter{equation}{0}
To further clarify the difference between the adiabatic bulk dipole moment (following the modern theory of polarization) and the impurity dipole moment $\textbf{D}^{\text{imp}}$ introduced in this paper, we consider a toy model with a parabolic dispersion:
\begin{equation}\label{D1}
H=\frac{(p_x-a_x)^2}{2m_x}+\frac{p_y^2}{2m_y}
\end{equation}
The parameter $a_x$ plays a similar role as the tilt $\delta v_x$ in the Dirac Hamiltonian.

Now, apply a magnetic field $B\hat{z}$ on the system. Denote a Landau orbital as $\ket{\psi}$ for $a_x$=0, and the corresponding Landau orbital when $a_x$ is tuned from zero to some finite value as $\tilde{\ket{\psi}}$. According to the polarization theory based on Berry phase, the difference of polarization between these two Landau orbitals is:
\begin{equation}\label{D2}
\begin{split}
\Delta D_y &= -\abs{e}l^2[\tilde{\bra{\psi}}\;p_x\;\tilde{\ket{\psi}}-\bra{\psi}p_x\ket{\psi}]\\
&=-\abs{e}l^2[ \tilde{\bra{\psi}}\;\tilde{p}_x+a_x\;\tilde{\ket{\psi}}-\bra{\psi}p_x\ket{\psi}]\\
&=-\abs{e}l^2[\tilde{\bra{\psi}}\;\tilde{p}_x\;\tilde{\ket{\psi}}-\bra{\psi}p_x\ket{\psi}+a_x]\\
&=-\frac{a_x}{\abs{B}}
\end{split}
\end{equation}
The last equality is obtained because $\tilde{p}_x=p_x-a_x$ is just a gauge transformation, while the expectation value $\bra{\psi}p_x\ket{\psi}$ should be gauge-invariant.

However, this dipole moment does not reflect the inversion asymmetry of the Landau orbital. In this example, there is simply no inversion asymmetry to begin with, and this can be verified if one examine ${\bf D}^{\rm imp} = e\langle \phi| {\bf  r}|\phi\rangle$, for the Landau orbital bound to a delta-potential impurity. By a proper gauge transformation, one can move the center of unperturbed Landau orbitals to the impurity site, irrespective of what $a_x$ is. After all, the presence of $a_x$ can be viewed as a gauge-transformation. In the presence of a delta-function impurity, only one state in each Landau level is bound to the impurity. That is the state $\phi_{n,n}$, which has a non-zero amplitude at the origin where the impurity sits.  As this state is inversion symmetric, and the perturbation (i.e. the delta potential) preserves this symmetry, the bound state should also be inversion symmetric. Thus $\bf D^{\rm imp}=0$.

In this extreme example, which can be considered as the parabolic limit ($\lambda \rightarrow \infty$) of the Dirac Hamiltonian, $\bf D$ measures solely the effect of Landau orbital displacement, which cannot be detected in a quantum Hall system due to edge screening. On the other hand, $\bf D^{\rm imp}$ measures only the inversion asymmetry of Landau orbitals, and therefore gives a local experimental signature for quantum Hall ferroelectrics. \\

\subsection{Numerical Setup of Exact Diagonalization}\label{E}
\setcounter{equation}{0}
\subsubsection{Anisotropic parabolic dispersions}

To exact-diagonalize the Hamiltonian with Coulomb interaction, one has to project the Coulomb term onto the Landau orbitals. In the main text, we deal with Landau levels arising from the tilted Dirac cones dispersion, while in this appendix we will also consider the case with parabolic dispersion. The parabolic case is the cornerstone for case with tilted Dirac cones dispersion, since the Dirac Landau orbitals are spinors consisting of parabolic Landau orbitals. The parabolic dispersion Hamiltonian is:
\begin{equation}\label{parabolic}
H=\frac{1}{2m^*}p_a g_{ab}p_b=\frac{1}{l_B^2m^*}(a^\dagger a+\frac{1}{2})
\end{equation}
where $p = \nabla/i-eA$, $g = Q^T S^2 Q$ is a $2\times 2$ tensor,  $Q\in SO(2)$ describes the rotation around principal axes in real space, the valleys we are interested in are vertical oriented, so we can set the real space axes along the principal axes of rotation, thus $Q=I$, and simply $g=S^2$. $S = diag\{(m_x/m_y )^{1/4}(m_y /m_x )^{1/4} \} $ is the mass tensor for the valley , effective mass $m^* = (m_x m_y )^{1/2}$. We introduce the mass ratio: $\alpha=m_x/m_y$ that specifies aspect ratio of the valley. The rescaled momenta along the principal axes of the tensor $\pi_a = S_{ab}p_b$ satisfy:
\begin{equation}
[\pi_a,\pi_b]=i l_B^{-2}\epsilon_{ab}
\end{equation}
and the LL lowering operator is:
\begin{equation}\label{momentum}
a=\frac{l_B}{\sqrt{2}}(\pi_x+i\pi_y),\quad [a,a^\dagger]=1
\end{equation}
Numerically, the electrons are on the 2D surface of torus, $L_x(L_y)$ represents the circumference of the torus along $x(y)$ direction and they satisfy relation $L_xL_y=2\pi N_0$, $N_0$ represents the number of orbitals for each valley.

Choosing the Landau gauge, $\vec{A}=(0,x)B$, the wavefunction of LL orbital is expressed as:\\
\begin{equation}
\begin{split}
\phi_{n,j}^\alpha&(r)=\left(\frac{2\pi}{L_yl_B}\right)^{1/2}\Sigma_{k=-\infty}^{+\infty}\overline{H_n}\left[\frac{x-k L_x-X_j}{\alpha^{1/4}l_B}\right]\times\exp[i(X_j+k L_x)y/l_B^2-(X_j+k L_x-x)^2/(2 \alpha^{1/2}l_B^2)]\\
\end{split}
\end{equation}
where $X_j=\frac{2\pi l_0^2 j}{L_y}$ to fulfill the periodic boundary condition, $\overline{H_n}$ is the physicist's Hermite polynomial that has been normalized so that:
\begin{equation}
\int^{+\infty}_{-\infty} \left(\overline{H_n}(x)\right)^2 e^{-x^2}dx=1
\end{equation}

With $\phi^\alpha_{n,j}(r)$ normalized as $\int_0^{L_y}dy\int_0^{L_x}dx|\phi_{n,j}^\alpha(r)|^2=2\pi$, when a Landau level is completely filled and thus the electron density is uniformly distributed, $\int_0^{L_y}dy\int_0^{L_x}dx\sum_j |\phi_{n,j}^\alpha(r)|^2=2\pi N_0=L_x L_y$ would then imply $\sum_j |\phi_{n,j}^\alpha(r)|^2=1$.

Next, we define $f_{nm}$ as the form factor for the parabolic Landau levels calculated in the Landau gauge:
\begin{equation}\label{factor}
\begin{split}
f_{nm}(\textbf{q}^\alpha)  &=\langle n,\alpha|e^{il_B^2\textbf{q}^\alpha\cdot\bm{\pi}}|m,\alpha\rangle \\
&=e^{-l_B^2(q_y^\alpha)^2/4}\int_{-\infty}^{+\infty}\overline{H_m}(x-\frac{q^\alpha_y}{2})\overline{H_n}(x+\frac{q^\alpha_y}{2})e^{-x^2}e^{iq^\alpha_x x}dx
\end{split}
\end{equation}
where the wavevector $\textbf{q}^\alpha$ is not the natural wavevector $\textbf{q}$ but rotated as
\begin{equation}
\textbf{q}^\alpha = -S^{-1}\epsilon\textbf{q}
\end{equation}
where $\epsilon$ is the rank-2 levi-civita symbol, $Q$ and $S$ are the matrices associated with the mass ratio $\alpha$. This definition will become clear later when we project the electron interaction on the LLs.
\subsubsection{Tilted Dirac cone dispersion}
The massless Dirac Hamiltonian is just Eq. (\ref{dirac}) with $\lambda=0$.
Similar to the case with a parabolic Hamiltonian in Eq. (\ref{parabolic}), here we would define $S=diag\{ (v_x/v_y)^{1/2},(v_y/v_x)^{1/2}\}$ and rescale the momentum by $\pi_a = S_{ab}p_b$, which explains Eq. (\ref{rescaledmomentum}). One can relate the mass ratio $\alpha$ in the anisotropic parabolic dispersion and velocity ratio $r=v_x/v_y$ in the Dirac dispersion as: $\alpha=r^2$.

Tilting of the Dirac cone along the $x$-direction is described by the following perturbation:
\begin{equation}
H_1=\delta v_x p_x=\delta v_x\sqrt{\frac{v_y}{v_x}}\frac{(a+a^\dagger)}{\sqrt{2}l_B}=\tau\frac{\sqrt{2}v}{l_B}(a+a^\dagger)
\end{equation}
where $\tau=\delta v_x/(2 v_x)$. Using the general expression for the tilted Dirac LL in Eq. (\ref{tiltedDirac}), we have the following expression for the $n=+3$ Dirac Landau level:
\begin{equation}
\begin{split}
|+3,\tau\rangle=\frac{1}{\sqrt{2}}\left(\begin{matrix}|3\rangle+\tau(-4\sqrt{3}|4\rangle+5|2\rangle)\\ |2\rangle+\tau(2\sqrt{6}|1\rangle-7|3\rangle)\end{matrix}\right)
\end{split}
\end{equation}
Here, for simplicity, we have suppressed the intra-Landau level indices and the mass ratio $\alpha$ that would label the parabolic Landau orbitals. The form factor for the Dirac Landau level is then obtained as follows:
\begin{equation}\label{Dfactor}
\begin{split}
F^3(\textbf{q}^\alpha,\tau)&=\langle +3,\tau|e^{il_B^2\textbf{q}^\alpha\cdot\bm{\pi}}|+3,\tau\rangle \\ &=\frac{1}{2}[f_{33}+f_{22}-2\tau(f_{32}+f_{23})-4\sqrt{3}\tau(f_{34}+f_{43})+2\sqrt{6}\tau(f_{12}+f_{21})]
\end{split}
\end{equation}
where $f_{nm}$ is the form factor for the parabolic Landau levels (Eq. \ref{factor}).

\subsubsection{Impurity potential}
The impurity potential is $U(\textbf{r})=V_0l_B^2\delta(\textbf{r})$.
The matrix elements of impurity potential projected to the $n$-th and $m$-th parabolic Landau levels are:
\begin{equation}
\begin{split}
U&^\alpha_{j_1,j_2,n,m
=V_0\frac{2\pi l_B}{L_y}\Sigma_{l=-\infty}^{+\infty}\Sigma_{k=-\infty}^{+\infty}\overline{H_n}\left[\frac{X_{j_1}+lL_x}{l_B\alpha^{1/4}}\right]\times\overline{H_m}\left[\frac{X_{j_2}+kL_x}{l_B\alpha^{1/4}}\right]e^{-\frac{(X_{j_1}+l L_x)^2+(X_{j_2}+k L_x)^2}{2l_B^2\sqrt{\alpha}}}
\end{split}
\end{equation}
In the parabolic dispersion case, one only need to consider the case $n=m$, and in the main text we focus on the lowest Landau level, so $n=m=0$; on the other hand, in the tilted Dirac case there exist non-trivial terms with $n\neq m$, the impurity matrix elements $\langle +3,\tau|\hat{U}(\textbf{r})|+3,\tau\rangle_{j_1,j_2}$ are linear combinations of $U_{j_1,j_2,n,m}$ with $n,m=1,2,3,4$, which is similar to the form factor in Eq. (\ref{Dfactor}).

\subsubsection{Coulomb interaction}
The Coulomb interaction in a finite system has the form
\begin{equation}
V(\textbf{r})=\frac{1}{L_x L_y}\sum_\textbf{q} V(q) e^{i \textbf{q}\cdot \textbf{r}}
\end{equation}
where $V(q)=\frac{2\pi e^2}{\epsilon q}$, for finite size torus with the circumference $L_x$ and $L_y$. Here $\textbf{q}=(\frac{2\pi s}{L_x},\frac{2\pi t}{L_y})$ takes discrete values to ensure the periodicity.

The projected Coulomb interaction between two electrons in the valleys $i$ and $j$ ($i,j$ can either be the same valley or two different valleys) into the $n$-th Landau level has the form:
\begin{equation}
\begin{split}
P_n &V(\textbf{r}_i-\textbf{r}_j)P_n=\frac{1}{L_xL_y}\sum_\textbf{q} V(\textbf{q}) F^n_i(\textbf{q}_i) F_j^{n}(\textbf{q}_j)^*e^{i \textbf{q}\cdot (\textbf{R}_i-\textbf{R}_j)}
\end{split}
\end{equation}
Here we have introduced the guiding center operator $\textbf{R}_{i}$ for valley $i$, which is related to the position operator as follows:
\begin{equation}
\textbf{r}_i \equiv \textbf{R}_i-l_B^2\epsilon\textbf{p}_i =  \textbf{R}_i-l_B^2\epsilon S_i^{-1}\bm{\pi}_i
\end{equation}
where $\epsilon$ is the rank-2 levi-civita symbol and $S_i$ is the $S$ tensor associated to valley $i$, which has been defined earlier for both parabolic and Dirac dispersions. Accordingly, wavevector $\textbf{q}_i$ is defined as:
\begin{equation}
\textbf{q}_i = -S_i^{-1}\epsilon\textbf{q}
\end{equation}
For the numerical results presented in the main text, the valleys have the same velocity ratio $r$ (or mass ratio $\alpha=r^2$) and opposite $\tau$. Thus we have $\textbf{q}_i=\textbf{q}_j=\textbf{q}^\alpha, F_{i/j}^n(\textbf{q}^\alpha)=F^3(\textbf{q}^\alpha,\pm\tau)$.  While for the numerics to be presented in the next section for anisotropic parabolic dispersion at $n=0$ LL, different valleys have different mass ratio $\alpha$ and $\beta$, where $\beta=\frac{1}{\alpha}$ for the two orthogonal-orientated valleys of interest. There we have $\textbf{q}_{i/j}=\textbf{q}^{\alpha/\beta}$, and $F^n_{i/j}=f_{00}$.\\

\subsection{Quantum Hall Nematics with Anisotropic Parabolic Dispersions}\label{F}
 After considering electron-electron interaction in ferroelectric states in the main text, here we illustrate a simpler scenario where the anisotropic parabolic dispersion is used so that the impurity only hosts a single bound state. The two valleys A and B are parabolic dispersive with the same aspect ratio, but vertical elliptical axes, meaning that if we choose the principal axes along the same direction for two valleys, there mass ratio will satisfy $\alpha=\frac{1}{\beta}$.  A smaller system size with $N_0=20$ single-valley orbitals is enough to demonstrate this case. The corresponding energy spectra with disorder are shown in Fig. \ref{paraspectrum}, and some representative tunneling density profiles are shown in Fig. \ref{paratunneling}, with various mass ratios. Again, just like what happens in the ferroelectric state around an impurity, when the impurity potential is larger than a certain threshold a quasihole state becomes the new ground state. Adding an electron to this state would lead to an exciton state, and the resulting density profile can be captured by STM measurements.
\begin{figure}[H]
\centering
\includegraphics[width=0.4\textwidth]{spectrumallinone2}
\caption{The energy spectra with increasing impurity potentials, as indicated in the legend, blue lines represent $\{N_0,0\}$, red lines $\{N_0,1\}$, orange lines $\{N_0-1,0\}$, purple lines $\{N_0-1,1\}$ and green lines $\{N_0-2,0\}$.  The mass ratios($\alpha=m_x/m_y$) in panels (a),(b),(c),(d) are $1,2,4,8$, respectively. The orbital number $N_0=20$. }
\label{paraspectrum}
\end{figure}

\begin{figure}[H]
\centering
\includegraphics[width=0.4\textwidth]{tunneling2.png}
\caption{The tunneling matrix elements from the ground state $\{N_0-1,0\}$ to the excitonic state $\{N_0-1,1\}$ for different mass ratio: $\alpha=2$ in (a, b) and $\alpha=8$ in (c,d),  which are proportional to the differential conductance obtained by direct STM measurements. The strength of impurity potential is set to be $0.6\frac{e^2}{2l_B^2N_0}$ and the length scale is in the unit of $l_B$.}
\label{paratunneling}
\end{figure}

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text:
Evasterias är ett släkte av sjöstjärnor. Evasterias ingår i familjen trollsjöstjärnor.

Kladogram enligt Catalogue of Life:

Bildgalleri

Källor

Externa länkar

Trollsjöstjärnor
Evasterias

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Here is the ideal tankini for the fuller bust! Designed to flatter, you'll love the security of structure and support in Shake, by the pool or on your sunny getaway by the beach. With flexible wire that is cut to sit under and around, you'll be astounded!


text:
Monday, January 17, 2022Jan 17, 2022
The Student Newspaper of Highline College
Highline Foundation opens student scholarship applications
The Highline College Foundation has opened applications for its 2021-2022 student scholarships.
Students can fill out a single online application to apply for the several Foundation scholarships on offer. Part-time, full-time, transfer, incoming, international, and undocumented students are all eligible to apply.
Highline Foundation Gala goes virtual for 2021
The Highline College Foundation's annual gala will be held virtually for the first time this April.
A nonprofit organization of the college, the Foundation has traditionally held the annual fundraising event at the Cedarbrook Lodge in SeaTac. Last year, in light of the emerging COVID-19 pandemic, it had to be cancelled on short notice.
The Highline Women's Program is again selling holiday wreaths and garlands in order to support students in need.
The Women's Program is a program helps primarily low-income students who need support services and guidance to achieve academic and educational goals through services and provided resources.
New trustee extends himself towards Highline community
Newly appointed Board of Trustees member Joe Bowman says he is ready to extend himself to the Highline community and support students better.
Bowman's appointment was announced Oct. 21, He replaces longtime trustee Bob Roegner, who is leaving the board after two terms.
Foundation raises funds to help students amid pandemic
Despite its annual gala being cancelled, the Highline College Foundation has managed to raise more than $150,000 for students in need.
Josh Gerstman, its executive director, says that students' need for support during this pandemic is what keeps him and the Foundation going.
Thunderword 2020
(206) 592-3317 Highline College 2400 S. 240th St. Des Moines, WA 98198

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Join us at the #PCTO14 Sat night after party!
Feeling energized after a day of sessions? You need to burn that energy. Join us at our annual Saturday evening after party. There's free food. And booze!
This year's party will once again be at Lou Dawg's (@LouDawgsRyerson), located at 78 Gerrard Street East, just one block north of the Rogers Communications Centre where #PCTO14 is taking place.
– Food is served at: 6:30 and 8:30 p.m.
Daryl D'Souza, the owner and general manager of Lou Dawg's who's no stranger to incorporating social media to the restaurant brand, is thrilled to play host for the #PCTO14 after-party. We thank Daryl and Lou Dawg's for sponsoring PodCamp Toronto and hope to see you all there!


text:
SolarEdge acquires controlling stake in battery provider Kokam
Israeli solar energy company SolarEdge Technologies announced on 11 October that it has entered into definitive agreements to acquire a controlling stake in South Korean company Kokam, which provides lithium-ion battery cells, batteries and energy storage solutions.
Kokam provides battery solutions for a wide variety of industries, including ESS (energy storage systems), UPS, electric vehicles (EV), aerospace, marine and more.
SolarEdge founder, chairman and CEO Guy Sella, said: "The acquisition of Kokam will enable us to grow our offering, adding already proven battery storage to our product portfolio. Our technological innovation, combined with Kokam's worldclass team and renowned battery storage solutions, will enable seamless integration with our current solutions, taking us a further step toward making solar installations smarter and more beneficial."


text:
The Rhythm of the Night is een nummer van de Italiaanse band Corona. Het is de eerste single van hun gelijknamige debuutalbum uit 1993. Het nummer werd op 5 november van dat jaar oorspronkelijk uitgebracht op single, maar werd toen géén hit.

"The Rhythm of the Night" werd in de zomer van 1994 opnieuw uitgebracht en werd toen een wereldwijde danshit en ook veruit de grootste hit voor Corona. De single haalde de nummer 1-positie in hun thuisland Italië. In de Verenigde Staten werd de 11e positie bereikt in de Billboard Hot 100, in Nieuw-Zeeland de 7e en in Australië de 8e positie. In het Verenigd Koninkrijk werd de 2e   positie in de UK Singles Chart bereikt.

In Nederland werd de single destijds veel gedraaid op Radio 538 en Radio 3FM en werd een grote hit. De single bereikte de 6e positie in de Nederlandse Top 40 op Radio 538 en de 4e positie in de destijds nieuwe publieke hitlijst op Radio 3FM; de Mega Top 50.

In België bereikte de single de 13e positie in de Vlaamse Ultratop 50 en de 20e positie in de Vlaamse Radio 2 Top 30.

Single uit 1994
Nummer van Corona


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text:
Vanderbilt could be the superior team against Tennessee — change my mind
Tennessee and Vanderbilt on Saturday should be aggressive — like brawling over blenders and toys after rushing a business on Black Friday aggressive
Vanderbilt could be the superior team against Tennessee — change my mind Tennessee and Vanderbilt on Saturday should be aggressive — like brawling over blenders and toys after rushing a business on Black Friday aggressive Check out this story on knoxnews.com: https://www.knoxnews.com/story/sports/college/university-of-tennessee/football/2019/11/29/tennessee-football-vanderbilt-could-be-better-team-change-my-mind/4319451002/
Ryan Wilusz, Knoxville News Sentinel Published 5:00 a.m. ET Nov. 29, 2019
I know we're all Vols fans here, but let's not forget there are two sides to every story.
The Tennessee and Vanderbilt game on Saturday should be aggressive — like brawling over blenders and toys after rushing a business on Black Friday aggressive.
And if there was one last stuffed Baby Shark on the top shelf of a Target, Vanderbilt would trample Tennessee and grab it — because Vandy has the ability to take care of business on what's sure to be a Black and Gold Saturday.
All of these Vanderbilt graduates who went on to lead successful businesses prove it.
Tennessee vs Vanderbilt football through the years
Tennessee's Richard Cooper (77) and Marr Houanic (59) tackle Vanderbilt's Eric Jones in the fourth quarter on November 28, 1988. J. Miles Cary J. Miles Cary/Knoxville News Sentinel
In a Nov. 29, 1997, photograph, Tennessee quarterback Peyton Manning scores the winning touchdown in a 17-10 victory over Vanderbilt during his final game at Neyland Stadium. Michael Patrick/News Sentinel
Vanderbilt coach Bill Pace, left, and Tennessee coach Bill Battle meet in the middle of the field for the traditional exchange of condolences and congratulations after the Vols 30-10 victory Dec. 2, 1972. Joe Rudis / The Tennessean
Tennessee quarterback Peyton Manning is pressured by Vanderbilt defenders on Nov. 29 1997, at Neyland Stadium. Manning went 12-27 passing with one interception and one touchdown as the Vols eked out a 17-10 victory. Bryon Small/News Sentinel
Tennessee defensive end Derek Barnett (9) chases down Vanderbilt quarterback Kyle Shurmur (14) during the first half at Neyland Stadium in Knoxville, Tenn. on Saturday, Nov. 28, 2015. MICHAEL PATRICK/NEWS SENTINEL
UT's Gerald Riggs, Jr. pushes off Vanderbilt's Andrew Pace on 11/20/04. Amy Smotherman/News Sentinel
Jessee Sanders (22), George Kidd (42), Scott Galyon (93) shut down Vanderbilt's Jermaine Johnson on November 25, 1995. Margaret Bentlage/Knoxville News Sentinel
During the fourth quarter, Vol Mark Fletcher foils Vanderbilt's only chance to score by batting the ball away from intended receiver Derrick Gragg on November 30, 1991. Patrick Murphy-Racey/Knoxville News Sentinel
Vanderbilt quarterback Steve Burger (10) fires a pass as his teammate blocks Tennessee defensive end Manley Mixon (46). The Sugar Bowl-bound Vols defeated the Commodores 24-6 before 33,850 at Dudley Field Nov. 28, 1970. Jack Corn / The Tennessean
Vanderbilt's Derrick Payne has his feet cut out from under him as Tennessee's Jesse Sanders closes in on November 28, 1992. Paul Efird/Knoxville News Sentinel
Tennessee's Jay Graham breaks through Vanderbilt's Marcus Williams, left, and Carlton Hall. Margaret Bentlage/Knoxville News Sentinel
Vanderbilt receiver Brandon Smith was able to catch the ball but came down hard and wasn't able to hold on to it during action against Tennessee at the Adelphia Coliseum Nov. 23, 2002. Larry McCormack / The Tennessean
Jim McDonald, Tennessee Head Coach, after a game against Vanderbilt in 1963. News Sentinel Photo Archive
Vanderbilt Head Coach Derek Mason during second quarter of their game against Tennessee at Neyland Stadium Saturday, Nov. 25, 2017 in Knoxville, Tenn.. Michael Patrick/News Sentinel
Tennessee running back Alvin Kamara (6) runs the ball against Vanderbilt during the second half at Neyland Stadium in Knoxville, Tenn. on Saturday, Nov. 28, 2015. ADAM LAU/NEWS SENTINEL
James Stewart stays on his toes as he weaves through the Vanderbilt defense on November 28, 1992. Paul Efird/Knoxville News Sentinel
Tennessee quarterback Peyton Manning takes the field for his last home game on Saturday, Nov. 29, 1997 in Knoxville, Tenn. Tennessee defeated Vanderbilt 17-10. MARK HUMPHREY/ASSOCIATED PRESS NFS
UT's Arian Foster knocks off the helmet of Vanderbilt's Kelechi Ohanaja (12) in the first half of the game at Neyland Stadium Saturday afternoon. Foster finished the game with 40 carries for 223 yards and 2 touchdowns on 11/19/2005. Jeff Adkins/Knoxville News Sentinel
Tennessee running back Alvin Kamara (6) leaps over Vanderbilt safety Ryan White (14) during the first half at Vanderbilt Stadium on Saturday, Nov. 26, 2016. Vanderbilt won the game 45-34. AMY SMOTHERMAN BURGESS/NEWS SENT
Greg Master dives over the top for a first down in 1988. News Sentinel Photo Archive
Marcus Wilson goes for the ball during action against Tennessee on November 28, 1992. Paul Efird/Knoxville News Sentinel
Tennessee vs Vanderbilt action on November 26, 1982. News Sentinel Photo Archive
Vanderbilt quarterback Jay Cutler, left, talks with Tennessee defensive tackle Jesse Mahelona at Neyland Stadium Saturday after the Commodores' 28-24 victory on 11/19/2005. Jeff Adkins/Knoxville News Sentinel
Tennessee's Haskel Stanbeck (24) is attacked by Vanderbilt defense on December 2, 1972. News Sentinel Photo Archive
Lee England fumbles the snap on a field goal attempt with Vanderbilt's Derrick Payne (24) making the tackle in 1988. News Sentinel Photo Archive
UT head coach Phil Fulmer watches as his team loses to Vanderbilt at Neyland Stadium Saturday afternoon on 11/19/2005. Jeff Adkins/News Sentinel
Sixty-five thousand people, largest crowd ever to gather for a single program in Tennessee, fill Vanderbilt stadium Sept. 19, 1954. During the last night of the Greater Nashville Crusade, 1,121 people answered the invitation of Billy Graham to be witnesses for Christ. Gerald Holly / The Tennessean
Tennessee's John Emery (46) takes down Vanderbilt's Eric Lewis (22) on November 27, 1993. Michael Patrick/Knoxville News Sentinel
Tom Redmond (72), Ross Morris (44) and Don Deck (89) during action against Vanderbilt on November 30, 1958. News Sentinel Photo Archive
Clarence Sullivan gets a hug after one of three touchdown catches on November 28, 1992. He had six receptions for 222 yards. Paul Efird/Knoxville News Sentinel
The Commodores fumbled the ball twice and the Vols managed to recover one on on November 28, 1992. Paul Efird/Knoxville News Sentinel
A Heath Shuler pass slips through the fingertips of Tennessee wide receiver Cory Fleming on on November 28, 1992. Paul Efird/Knoxville News Sentinel
Tennessee running back Alvin Kamara (6) is congratulated after scoring the first touchdown of the game during the first half at Vanderbilt Stadium on Saturday, Nov. 26, 2016. AMY SMOTHERMAN BURGESS/NEWS SENT
Craig Faulkner gave the Vols a lift by scoring a touchdown against Vanderbilt on on November 28, 1992. Paul Efird/Knoxville News Sentinel
A pair of Vanderbilt cheerleaders support their Commodores on Sept. 13, 1975. Frank Empson / The Tennessean
UT's Arian Foster (27) gets chased down by Vanderbilt defenders at Neyland Stadium Saturday afternoon on 11/19/2005. Adkins, Jeff/Knoxville News Sentinel
Tennessee's Joey Kent (11) gains yardage before Vanderbilt's Fred Vinson (1) comes information the tackle on November 25, 1995. Margaret Bentlage/Knoxville News Sentinel
Tennessee's David Horn, left, makes a hard hit on Vanderbilt's Eric Vance on November 26, 1994. Clay Owen/Knoxville News Sentinel
Vanderbilt quarterback Kyle Shurmur (14) passes the ball against Tennessee during the second half at Neyland Stadium in Knoxville, Tenn. on Saturday, Nov. 28, 2015. News Sentinel Photo Archive
Tennessee quarterback Peyton Manning is greeted by Vol mascot Smokey before the Vanderbilt game Nov. 29, 1997, at Neyland Stadium. It was Manning's final home game. Byron Small/News Sentinel
Players celebrate during the first half at Vanderbilt Stadium on Saturday, Nov. 26, 2016. AMY SMOTHERMAN BURGESS/NEWS SENT
Vanderbilt's Kenny Simon (6) and Tennessee's Raymond Austin during game action on November 25, 1995. Margaret Bentlage/Knoxville News Sentinel
Fans say thanks to Tennessee quarterback Peyton Manning during the Vanderbilt game on Saturday, Nov. 29, 1997, at Neyland Stadium. The Vols prevailed 17-10 in Manning's last home game. Michael Patrick/News Sentinel
Vanderbilt tailback Lonnie Sadler carries the ball into the line and plows under Tennessee defender Robert Pulliam (70) as the Commodores' Dave Alsup (63) throws a block. Tennessee kicked two field goals late to win 20-17 before 66,702 at Neyland Stadium in Knoxville Dec. 1, 1973. Jimmy Ellis / The Tennessean
Tennessee's Steve White is held off by Vanderbilt's Allen DeGraffenreid as Vanderbilt's Duane Todd recovers a loose ball in the first quarter of Saturday's game on November 26, 1994. Clay Own/Knoxville News Sentinel
Tennessee fans cheer on the team against Vanderbilt during the second half at Neyland Stadium in Knoxville, Tenn. on Saturday, Nov. 28, 2015. MICHAEL PATRICK/NEWS SENTINEL
Condredge Holloway, Tennessee sophomore quarterback (7) scampers around against Vanderbilt Dec. 2, 1972. Looking on are Vanderbilt's Mark Llewellyn (87), UT's David Shafer (77) and Mike Kirk (75) and George Abernathy (89), both of Vanderbilt. The Vols won 30-10 before 34,000 fans at Dudley Field in Nashville. Robert Johnson / The Tennessean
Vanderbilt quarterback Ronnie Gordon (3) was pressed by Tennessee's defense all day. Tennessee's Shane Boham reaches for Gordon during first half play on November 27, 1993. Michael Patrick/Knoxville News Sentinel
Vanderbilt quarterback Kyle Shurmur (14) during second quarter of their game against Vanderbilt at Neyland Stadium Saturday, Nov. 25, 2017 in Knoxville, Tenn.. Michael Patrick/News Sentinel
Vanderbilt's quarterback Damian Allen gets sacked by Tennessee's Steve White on November 25, 1995. Joe Howell/Knoxville News Sentinel
Tennessee junior quarterback Steve Alatorre (16) attempts to hit an open receiver against Vanderbilt. The Vols defeated the Commodores 51-13 before 35,100 fans at Dudley Field Nov. 29, 1980. J.T. Phillips / The Tennessean
Tennessee defensive back Cameron Sutton (7) returns a punt for 85 yards against Vanderbilt during the first half at Neyland Stadium in Knoxville, Tenn. on Saturday, Nov. 28, 2015. ADAM LAU/NEWS SENTINEL
Tennessee linebacker Jalen Reeves-Maybin (21) reacts after a play against Vanderbilt during the second half at Neyland Stadium in Knoxville, Tenn. on Saturday, Nov. 28, 2015. (ADAM LAU/NEWS SENTINEL) ADAM LAU, ADAM LAU/NEWS SENTINEL
College football fans huddle under a canopy of umbrellas and plastic sheets as they react to the Vanderbilt and Tennessee game at Dudley Field Nov. 30, 1974. Frank Empson / The Tennessean
Tennessee head coach Derek Dooley pulls linebacker Jacques Smith off the field during the game against Vanderbilt at Vanderbilt Stadium in Nashville on Saturday, Nov. 17, 2012. Amy Smotherman Burgess, AMY SMOTHERMAN BURGESS/NEWS SENTINEL
utvandy10.ASB#4741.JPG--SPORTS-- Tennessee quarterback Rick Clausen pauses before leaving the field after the 28-24 loss to Vanderbilt Saturday at Neyland Stadium in 2005. Amy Smotherman Burgess/News Sentinel
Vanderbilt players celebrate after defeating Tennessee in an NCAA college football game Saturday, Nov. 26, 2016, in Nashville, Tenn. Vanderbilt won 45-34. (AP Photo/Mark Humphrey) Mark Humphrey, AP
Tennessee defensive back Eric Berry (14) returns an interception for a touchdown against Vanderbilt at Vanderbilt Stadium in Nashville on Saturday. Amy Smotherman Burgess/News Sentinel
Tennessee coach Lane Kiffin reacts to a call Saturday, Nov. 21, 2009, as the Vols beat Vanderbilt 31-16 at Neyland Stadium. Adam Brimer/News Sentinel
Tennessee running back Charlie Fulton (12) is attempting to break free of a trio of Vanderbilt defenders, Bernie Kemple (15), Mike Giltner (85) and Noel Stahl (89), during the Volunteers 41-14 victory over the Commodores at Neyland Stadium in Knoxville Dec. 2, 1967. Jack Corn / The Tennessean
Tennessee cornerback Eric Berry (14) greets fans after the 31-16 win over Vanderbilt on Saturday, Nov. 21, 2009 at Neyland Stadium. Amy Smotherman Burgess/Knoxville News Sentinel
Tennessee running back Ty Chandler (3) makes his way through Vanderbilt defense during a game between Tennessee and Vanderbilt at Neyland Stadium in Knoxville, Tenn., on Saturday Nov. 25, 2017. Michael Patrick/News Sentinel
Tennessee linebacker A.J. Johnson (45) tackles Vanderbilt running back Wesley Tate (24) during the first half at Neyland Stadium in Knoxville on Saturday, Nov. 23, 2013. ADAM LAU/NEWS SENTINEL
Winning Tennessee coach Bowden Wyatt, left, talks with Vanderbilt coach Art Guepe, who concluded his decade of coaching for the Commodores, with a 30-0 defeat at Dudley Field Dec. 1, 1962. Jimmy Ellis / The Tennessean
Tennessee wide receiver Marquez Callaway (1) makes a touchdown as Vanderbilt corner back Tre Herndon (31) attempts to tackle him during a game between Tennessee and Vanderbilt at Neyland Stadium in Knoxville, Tenn., on Saturday Nov. 25, 2017. Michael Patrick/News Sentinel
Tennessee back Keith Davis (28) is bracing for the hit from Vanderbilt linebacker Chris Gaines (34). Davis picked up 73 yards on 12 rushing attempts. The Vols defeated the Commodores 30-0 before 97,372 at Neyland Stadium in Knoxville Nov. 30, 1985. Callie Shell / The Tennessean
Tennessee defensive back Shaq Wiggins (6) pumps up the crowd at the start of the fourth quarter during a game between Tennessee and Vanderbilt at Neyland Stadium in Knoxville, Tenn., on Saturday Nov. 25, 2017. Calvin Mattheis/News Sentinel
At center Vanderbilt corner back Joejuan Williams (8) celebrates with fans after the game against Vanderbilt at Neyland Stadium Saturday, Nov. 25, 2017 in Knoxville, Tenn.. Vanderbilt defeated Tennessee 42-24. Michael Patrick/News Sentinel
Tennessee defensive back Micah Abernathy (22) runs after Vanderbilt running back Ralph Webb (7) during the game against Vanderbilt at Neyland Stadium Saturday, Nov. 25, 2017 in Knoxville, Tenn.. Vanderbilt defeated Tennessee 42-24. Michael Patrick/News Sentinel
A Vanderbilt fan watches the game during a game between Tennessee and Vanderbilt at Neyland Stadium in Knoxville, Tenn., on Saturday Nov. 25, 2017. Calvin Mattheis/News Sentinel
Vanderbilt receiver Earl Bennett, center, is hit by Tennessee defenders Jerod Mayo, left, and Ryan Karl (39) after catching the ball. Tennessee edged Vanderbilt 25-24 at Neyland Stadium Nov. 17, 2007. Wade Payne / AP Photo
With his injured foot taped up, Tennessee quarterback Condredge Holloway (7) is back in the game and scrambles for yardage against Vanderbilt. Tennessee kicked two field goals late to win 20-17 before 66,702 at Neyland Stadium in Knoxville Dec. 1, 1973. Jimmy Ellis / The Tennessean
Vanderbilt linebacker Jordan Griffin (40) celebrates a play during a game between Tennessee and Vanderbilt at Neyland Stadium in Knoxville, Tenn., on Saturday Nov. 25, 2017. Calvin Mattheis/News Sentinel
Tennessee running back Mike Gayles (43) is heading up field against Vanderbilt as quarterback Condredge Holloway (7) looks on. The two teams finishes the game in a 21-21 tie at Dudley Field Nov. 30, 1974. Frank Empson / The Tennessean
Vanderbilt running back Ralph Webb (7) runs the ball during a game between Tennessee and Vanderbilt at Neyland Stadium in Knoxville, Tenn., on Saturday Nov. 25, 2017. Calvin Mattheis/News Sentinel
"Voice of the Vols" John Ward is recognized on the field during a game between Tennessee and Vanderbilt at Neyland Stadium in Knoxville, Tenn., on Saturday Nov. 25, 2017. Caitie McMekin/News Sentinel
Vanderbilt head coach Bill Pace, left, and Tennessee head coach Bill Battle exchange a greeting at the end of the hard fought game. The Sugar Bowl-bound Vols defeated the Commodores 24-6 before 33,850 at Dudley Field Nov. 28, 1970. Jack Corn / The Tennessean
Vanderbilt receiver Earl Bennett (10) pulls in a pass over Tennessee defensive back Inquoris Johnson (29), setting up the Commodores winning touchdown. Vanderbilt won 28-24 at Neyland Stadium Nov. 19, 2005. Billy Kingsley / The Tennessean
Tennessee head coach Bill Battle, left, and Vanderbilt head coach Steve Sloan trade congratulations following the 21-21 tie between their teams at Dudley Field Nov. 30, 1974. Frank Empson / The Tennessean
Vanderbilt head coach Jack Green, right, looks on with a couple of his players, including John Bruno (42) in what could be his last game as coach against Tennessee at Dudley Field Nov. 26, 1966. Joe Rudis / The Tennessean
Vanderbilt quarterback David Lee (8) gets slammed to the wet turf by Tennessee defenders Ron McCartney (57), David Poley (46) and David Page (72). The two SEC rivals finished the game in a 21-21 tie at Dudley Field in Nashville Nov. 30, 1974. Jimmy Ellis / The Tennessean
Tennessee running back Dale Fair makes a diving attempt to catch a pass against Vanderbilt. The two SEC rivals finished the game in a 21-21 tie at Dudley Field in Nashville Nov. 30, 1974. Jimmy Ellis / The Tennessean
Vanderbilt running back Alvin Duke (24) finds some running room against Tennessee. No. 9 ranked Tennessee won 17-10 at Neyland Stadium Nov. 29, 1997. Ricky Rogers / The Tennessean
Vanderbilt quarterback Jay Cutler (6) throws the winning touchdown in the closing minutes of play against Tennessee as Cassen Jackson-Garrison (22) protects Cutler. Vanderbilt won 28-24 at Neyland Stadium Nov. 19, 2005. Billy Kingsley / The Tennessean
NASHVILLE, TN - NOVEMBER 22: Eric Berry #14 of the Tennessee Volunteers rushes upfield against the Vanderbilt Commodores during the game at Vanderbilt Stadium on November 22, 2008 in Nashville, Tennessee. (Photo by Kevin C. Cox/Getty Images) Kevin C. Cox, Getty Images
Head coaches George MacIntyre of Vanderbilt, left, and Johnny Majors of Tennessee meet at mid-field after the game. The Vols defeated the Commodores 51-13 before 35,100 fans at Dudley Field Nov. 29, 1980. Frank Empson / The Tennessean
Tennessee linebacker Curt Maggitt (56) carries the UT flag onto the field to celebrate the Volunteers' 24-17 win at Vanderbilt that will send them to a bowl game for the first time since 2010. Larry McCormack / The Tennessean
Tennessee head coach Johnny Majors, left, and Vanderbilt head coach George MacIntyre greet at the end of a very tough game. The Vols survive 38-34 against the Commodores before 92,824 at Neyland Stadium Nov. 28, 1981. Frank Empson / The Tennessean
Tennessee cornerback Eric Berry (14) leaves the field possibly for the last time as the Vols defeat Vanderbilt 31-16 on Saturday, Nov. 21, 2009 at Neyland Stadium. News Sentinel Photo Archive
Tennessee senior quarterback Steve Alatorre (16) lets fly with a pass over the leaping Vanderbilt junior defensive end Bob O'Connor (83). Alatorre had a big game passing with 10 of 20 for 319 yards. The Vols survive 38-34 against the Commodores before 92,824 at Neyland Stadium Nov. 28, 1981. Frank Empson / The Tennessean
Tennessee receiver Donte Stallworth (4) keeps running as Vanderbilt defender Jerrol Jackson grabs him. Tennessee won 38-0 at Neyland Stadium Nov. 24, 2001. Larry McCormack / The Tennessean
Tennessee star running back Johnnie Jones (33) breaks free from the grab of a Vanderbilt defender in their game at Neyland Stadium in Knoxville Nov. 26, 1983. Jones, a junior, amassed 248 yards in 30 carries for the game and became UT's first single-season 1,000-yard rusher. The bowl-bound Volunteers defeated the Commodores 34-24 before 93,426 fans. Ricky Rogers / The Tennessean
Tennessee linebacker Jalen Reeves-Maybin (21) reacts after a play against Vanderbilt during the second half at Neyland Stadium in Knoxville, Tenn. on Saturday, Nov. 28, 2015. (ADAM LAU/NEWS SENTINEL) ADAM LAU
Almost hidden in the mass of humanity is Tennessee place kicker Carlos Reveiz (92) as he kicks a 23-yard first-quarter field goal against Vanderbilt. The Vols defeated the Commodores 30-0 before 97,372 at Neyland Stadium in Knoxville on Nov. 30, 1985. Ricky Rogers / The Tennessean
Christopher Hanewinckel, Christopher Hanewinckel-USA TODAY Sports
Vanderbilt split end Gerald "Boo" Mitchell (6) tries to escape the grasp of Tennessee defender Andre Creamer (1). Tennessee won 35-20 at Dudley Field Nov. 29, 1986 to finishes 6-5 and a trip to the Liberty Bowl. Ricky Rogers / The Tennessean
Vanderbilt's Everett Crawford (1) is attempting to plow through a host of Tennessee defenders, including Darrin Miller (45). Tennessee pulled out a 38-36 victory over Vanderbilt before 93,306 at Neyland Stadium in Knoxville Nov. 28, 1987. Rick Musacchio / The Tennessean
Tennessee tailback Reggie Cobb (34) is grabbed by Vanderbilt linebacker Chris Gaines (34) as he attempts to dive over the goal line for a touchdown during second-quarter action. Tennessee pulled out a 38-36 victory over Vanderbilt before 93,306 at Neyland Stadium in Knoxville on Nov. 28, 1987. Rick Musacchio / The Tennessean
Doug Mathews, 70: After playing running back at Vanderbilt, Mathews had a 20-year coaching career that included stops at Tennessee and Vanderbilt and retired in 1990. After a couple of years as Vanderbilt radio color analyst, Mathews is now host of "Football Saturday" and "Big Orange Sunday" on 104.5-FMand "Coach-to-Coach" on 30 stations across the state. Ricky Rogers / The Tennessean
In his last game leading the Vols, Tennessee head coach Johnny Majors waits to take the field against Vanderbilt on Saturday, Nov. 28, 1992, in Nashville. Assistant head coach Phillip Fulmer was introduced as Tennessee's new head coach the next day. KNS Archive, Paul Efird/News Sentinel
Vanderbilt running back Alvin Duke (20), is caught between Tennessee defenders Tori Noel (9) and Eric Lane (5) after a short gain. Tennessee won 14-7 at Dudley Field Nov. 30, 1996. Freeman Ramsey / The Tennessean
Tennessee running back Charlie Fulton (12) attempts to break free of a trio of Vanderbilt defenders, Bernie Kemple (15), Mike Giltner (85) and Noel Stahl (89), during the Volunteers' 41-14 victory over the Commodores at Neyland Stadium in Knoxville on Dec. 2, 1967. Jack Corn / The Tennessean
Tennessee defensive backs coach Willie Martinez and head coach Butch Jones, center from left, celebrate their 24-17 win over Vanderbilt with the team at Vanderbilt Stadium on Saturday, Nov. 29, 2014 in Nashville, Tenn. (ADAM LAU/NEWS SENTINEL) Adam Lau, ADAM LAU/NEWS SENTINEL
Tennessee receiver Johnny Mills (85) is catching the pass as Vanderbilt defenders Trow Gillespie (34) falls down and Bob Goodridge (35) looks on. Tennessee won 28-0 for their seventh win of the season before 26,882 at Dudley Field Nov. 26, 1966. Bill Preston / The Tennessean
Tennessee defensive back Micah Abernathy (22) breaks up a pass meant for Vanderbilt tight end Jared Pinkney (80) during the second half at Vanderbilt Stadium on Saturday, Nov. 26, 2016. Vanderbilt won the game 45-34. AMY SMOTHERMAN BURGESS/NEWS SENTINEL
Tennessee receiver Johnny Mills is heading for the end zone after catching a pass against Vanderbilt at Dudley Field Nov. 26, 1966. Jack Corn / The Tennessean
Tennessee backup quarterback Bubba Wyche (18) is throwing a pass after getting away from Vanderbilt defender Mike Dawson (65) Nov. 26, 1966. Jack Corn / The Tennessean
Tennessee quarterback Tyler Bray (8) throws an interception caught by Vanderbilt linebacker Archibald Barnes (15) at Neyland Stadium on Saturday, Nov. 19, 2011. UT won the game 27-21.(AMY SMOTHERMAN BURGESS/NEWS SENTINEL) Amy Smotherman Burgess, Knoxville News Sentinel
The Vanderbilt marching band cheers in the stands during a game between Tennessee and Vanderbilt at Neyland Stadium in Knoxville, Tenn., on Saturday Nov. 25, 2017. Calvin Mattheis/News Sentinel
Vanderbilt linebacker Dave Maddux (53) attempts to talk with monster man Chip Healy, who had been knocked unconscious in action against Tennessee at Dudley Field Nov. 26, 1966. Keeping an eye on Healy is team physician A. Brant Lipscomb, center. Joe Rudis / The Tennessean
Tennessee running back Cedric Houston (21) breaks through several Vanderbilt defenders to take the ball in for a touchdown. Tennessee edged Vanderbilt 38-33 at Dudley Field Nov. 20, 2004. Larry McCormack / The Tennessean
Vanderbilt defensive tackle Frank Curtin (64) is getting treatment from team physician A. Brant Lipscomb, left, after getting injury against Tennessee Nov. 26, 1966. Joe Rudis / The Tennessean
Vanderbilt's Cassen Jackson-Garrison (22) takes Jonathan Hefney (33) along for the ride as he picks up yardage while Tennessee plays Vanderbilt at Neyland Stadium in Knoxville on Nov. 19, 2005. Larry McCormack / Tennessean
Vanderbilt defensive backs John Gamble (25) and Bernie Kemple (15) looks on as the pass for Tennessee Austin Denney (84) was too long Nov. 26, 1966. Jack Corn / The Tennessean
Tennessee quarterback Erik Ainge (10) is attempting to get his throw past Vanderbilt linebacker Kevin Joyce (40). Tennessee won 39-10 at Dudley Field Nov. 18, 2006. Larry McCormack / The Tennessean
Vanderbilt head coach Jack Green, center, talks with his assistant coach and quarterback Roger May (12) in what could be his last game as coach against Tennessee at Dudley Field Nov. 26, 1966. Joe Rudis / The Tennessean
Tennessee offensive teammates Jerry Holloway (76), Bob Johnson (54) and Richard Pickens have a word before their next play against Vanderbilt at Dudley Field Nov. 26, 1966. Jack Corn / The Tennessean
Tennessee defensive lineman Curt Maggitt (56), linebacker A.J. Johnson (45) and linebacker Shane Reveiz (30) celebrate with one another after defeating Vanderbilt 27-21 in overtime at Neyland Stadium Saturday, Nov. 19, 2011. ADAM BRIMER/NEWS SENTINEL
With teammates Charlie Fulton (12) and Richard Pickens (34) blocking in front of him, Tennessee quarterback Dewey Warren (16) is ready to unload against Vanderbilt Nov. 26, 1966. Frank Empson / The Tennessean
Tennessee wide receiver Von Pearson celebrates a touchdown against Vanderbilt on Saturday, Nov. 28, 2015, at Neyland Stadium. (ADAM LAU/NEWS SENTINEL) ADAM LAU
Tennessee monster man Jim Glover (32) and a teammate are ready to dump Vanderbilt fullback Jim Whiteside (44) on the ground at Dudley Field Nov. 26, 1966. Bill Preston / The Tennessean
Tennessee head coach Doug Dickey, right, pats Vanderbilt head coach Jack Green on the shoulder as they meet on the field after their game at Dudley Field Nov. 26, 1966. Tennessee won 28-0 for their seventh win of the season before 26,882 at Dudley Field Nov. 26, 1966. Jack Corn / The Tennessean
Tennessee tackle William Brimfield (54) holds up a sign he got from a fan in the stands after Tennessee defeated Vanderbilt 20-10 at Dudley Field Nov. 22 2008. It is Tennessee head football coach Phillip Fulmer last season at the school. Larry McCormack / The Tennessean
Vanderbilt end Gary Hudson (86) can only twist in frustration as the ball is deflected over his head and out of reach by Tennessee defender Wayne Waff. Tennessee walloped the Commodores 30-0 before an estimated 25,500 fans at Dudley Field in Nashville in 1962. Jimmy Ellis / The Tennessean
Tennessee tight end Jason Croom (18) makes a catch during the first half at Vanderbilt Stadium on Saturday, Nov. 26, 2016. AMY SMOTHERMAN BURGESS/NEWS SENT
Shaker's Shocker, the 1966 World Champion of the Tennessee Walking Horse National Celebration, is making an appearance as a mascot for Tennessee in their game with Vanderbilt at Dudley Field in Nashville Nov. 26, 1966. Jack Corn / The Tennessean
Tennessee receiver Tony Brown can't bring the ball down for a touchdown over Vanderbilt defensive back Cheron Thompson (8) at Adelphia Coliseum Nov. 23, 2002. The Vols blanked the Commodores 24-0. Larry McCormack / The Tennessean
Vanderbilt halfback Bob Sullins (22) follows the block of teammate Paul Guffee (64) to score the only touchdown of the game against Tennessee on the two-yard run. Vanderbilt upset Tennessee 7-0 before an estimated 30,000 fans at Dudley Field Nov. 28, 1964. Bill Preston / The Tennessean
Tennessee back Cedrick Houston races through a large hole for a touchdown against Vanderbilt at Adelphia Coliseum Nov. 23, 2002. The Vols blanked the Commodores 24-0. Larry McCormack / The Tennessean
Vanderbilt head coach Jack Green is lifted high by his players as Tennessee head coach Doug Dickey, second from right, is caught in the mob. The Commodores upset Tennessee 7-0 before an estimated 30,000 fans at Dudley Field Nov. 28, 1964. It's Vanderbilt first victory over the Vols singe 1959 and its first at Dudley Field since 1951. Bill Preston / The Tennessean
Tennessee defensive back Baylen Buchanan (28) stops Vanderbilt wide receiver Amir Abdur-Rahman (87) just short of the endzone in the second half at Vanderbilt Stadium Saturday, Nov. 24, 2018, in Nashville, Tenn. George Walker IV / Tennessean.com
Vanderbilt players celebrate the 38-13 win over Tennessee at Vanderbilt Stadium Saturday, Nov. 24, 2018, in Nashville, Tenn. Calvin Mattheis / News Sentinel NFS
First, let me just say Tennessee sure is lucky it doesn't have to travel to Vanderbilt Stadium on Saturday. Vandy graduated the CFO of Delta Airlines, which is known to make its guests incredibly uncomfortable in small spaces.
The current chairman of Equifax also went to Vanderbilt, but Vandy fans have never had to worry about a breach. Security is so tight at the 40,000-person stadium that it looks like they didn't let anybody inside for last week's game.
Small crowd at Vanderbilt-East Tennessee State football game @VandyFootballpic.twitter.com/LBumfyZPyf
— Chip Cirillo (@ChipCirillo) November 23, 2019
But this week's game is at Neyland Stadium, where everyone is welcome – and that never made much sense to me. Do you really want 100,000 people watch you lose?
This is not just me speculating. I have insider information.
The CEO of Nasdaq is also a Commodore and, if we treat Vandy football like the stock market, I've discovered a possible upward trend. After defeating East Tennessee State last week, Vandy's winning percentage is upseven to 27%.
The Vols should be worried about this, especially since the Vanderbilt football team has an entire military behind it.
I'm not just talking Commodores. I'm talking about generals — Dollar General and General Motors, to be exact, which both have had Vanderbilt graduates lead the companies as president.
A Vandy fan cheers during the first half at Vanderbilt Stadium Saturday, Nov. 24, 2018, in Nashville, Tenn. (Photo: George Walker IV / Tennessean.com)
If you had a dollar for every win the Commodores have this season, you could probably buy anything you want in Dollar General or, at least, one of these General Motors cars – plus shipping.
The former president of Kodak is another Vanderbilt graduate, and fans should definitely take a picture during Saturday's game. Because just like with Snapchat, whose former COO is a Commodore, game day will only last 24 hours before the season is gone forever.
Unless, of course, you're going to a bowl game.
I could go on telling you all the reasons Vanderbilt is far superior to Tennessee but, perhaps, it's best to lest Saturday's game speak for itself.
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Vols' Pruitt doesn't dismiss possibility of Banks returning


Tadashi Shoji launched in 1982. Known for designing for all ages, all ethnicity and all figures; Shoji uses figure flattering techniques such as draping, ruching, and shutter pleats to emphasize the positives. This Tadashi Shoji Evening Dress is guaranteed authentic. It's crafted with Nylon/Cotton/Polyester.


text:
Feds Shut Down Website Peddling Phony COVID-19 Vaccine
As coronavirus scams multiply, DOJ issues tips to recognize and avoid them
by Katherine Skiba, AARP, March 23, 2020 | Comments: 0
The website promised free COVID-19 vaccines for a small shipping fee.
En español | Federal officials announced the shutdown of a newly created website peddling a "free" vaccine for COVID-19 for a $4.95 shipping fee. The website, created in early March, used a photo of Anthony Fauci, M.D., a prominent federal health official working overtime to fight the pandemic, to imply the U.S. government backed the effort.
No vaccine now exists for COVID-19. The federal case — the first of its kind since the outbreak erupted — was filed in Austin, Texas, after an FBI official there on March 19 visited the website offering the bogus vaccine. The website address, now disabled, was coronavirusmedicalkit.com.
Abuse your credit cards, steal your identity
The website sought credit card and personal information to make fraudulent purchases and commit identity theft, authorities said. In announcing Sunday that a federal judge in Texas issued an order to immediately shutter the site, the U.S. Department of Justice (DOJ) released important tips to help the public guard against known and emerging scams triggered by the coronavirus.
In this case, the phony vaccine was said to be from the World Health Organization (WHO), which does not have one. The vaccine was said to cost nothing, but potential recipients were told to pay a $4.95 shipping fee using a credit card.
Feds blast alleged fraudster as 'despicable'
People should report suspected fraud schemes tied to COVID-19 by calling the National Center for Disaster Fraud hotline at 866-720-5721, or emailing disaster@leo.gov.
—William Barr, U.S. attorney general
One DOJ official in the case assailed the defendant as among "the most despicable of scammers." An FBI official involved in what is an ongoing investigation said the bureau has made it a priority to protect communities from "reprehensible fraud schemes" meant to spread misinformation and create confusion during the pandemic.
The defendant in the case is "John Doe, also known as coronavirusmedicalkit.com."
Namecheap located in Phoenix, is the domain's registrar and as such allowed potential victims to access the site. DOJ officials on March 19 informed Namecheap of the fraudulent statements on the virus website, court documents show. As of Monday morning, the website was no longer accessible to the public.
"Namecheap is actively working with authorities to both proactively prevent, and take down any fraudulent or abusive domains or websites related to COVID-19 or the Coronavirus."
— Richard Kirkendall, Namecheap, Inc. CEO
Since 1984, Fauci has directed the National Institute of Allergy and Infectious Diseases. He often appears at White House briefings and in interviews, making him a recognizable name and face in the federal response to the pandemic.
The news Sunday came after Attorney General William Barr announced last week that fighting coronavirus scams is now a top priority for federal prosecutors across the U.S.
Feds urge vigilance against coronavirus scams
The Department of Justice urges Americans to guard against known and emerging scams tied to COVID-19:
Independently verify the identity of any company, charity or individual that contacts you regarding COVID-19.
Check the websites and email addresses offering information, products or services related to COVID-19. Be aware that scammers often employ addresses that differ only slightly from those belonging to the entities they are impersonating. For example, they might use "cdc.com" or "cdc.org" instead of the legitimate "cdc.gov."
Be wary of unsolicited emails offering information, supplies or treatment for COVID-19 or requesting your personal information for medical purposes. Legitimate health authorities will not contact the general public this way.
Do not click on links or open email attachments from unknown or unverified sources. Doing so could download a virus onto your computer or device.
Make sure the antimalware and antivirus software on your computer is operating and up to date.
Ignore offers for a COVID-19 vaccine, cure or treatment. If a vaccine becomes available, you won't hear about it for the first time through an email, online ad or unsolicited sales pitch.
Check online reviews of any firm offering COVID-19 products or supplies. Avoid firms whose customers have complained about not receiving what was ordered.
Research charities or crowdfunding sites soliciting donations. An organization may not be legitimate even if it uses words like "CDC" or "government" or has reputable-looking seals or logos.
Be wary of any business, charity or individual requesting payments or donations in cash, by wire transfer or gift card, or through the mail. Don't send money through any of these channels.
Be cautious of "investment opportunities" tied to COVID-19, especially those based on claims that a small firm's products or services can help stop the virus. Carefully research the investment beforehand and visit the Securities and Exchange Commission (SEC) website to learn more about avoiding investment fraud.
More on Scams and Fraud
Beware of these coronavirus scams
Crooks exploiting coronavirus fears, according to the Secret Service
In a shaky stock market, watch out for this scam


Thirunaal is an action film that stars Jiiva and Nayanthara in the lead roles under the direction of P.S.Ramnath of Ambasamudram Ambani fame.
Hero Jiiva, an orphan, works under gangster Sharath Lohitashwa, who keeps the townships of Thanjavur and Kumbakonam under his control. Heroine Nayanthara's father, Joe Malloori, is a business partner with Sharath. Amidst this situation, Nayanthara often gets a dream of Jiiva marrying her. So, whenever she happens to meet Jiiva, she feels afraid and leaves the place.
One day, a rowdy gang kidnap Nayanthara when she visits her neighbor Yogi Devaraj, who fails to repay a debt. During that incident, Jiiva fights with the gang single-handedly and saves Nayan. When he expresses his love towards her after the fight, Nayan accepts it and both of them start enjoying their days. Not being aware of this relationship, Joe Malloori fixes a bridegroom to Nayan and makes the arrangements for their engagement. The function comes to a halt when the love affair gets revealed.
Depressed about the happenings, Joe Malloori decides to return to his home town and asks Sharath to settle down his share. When Sharath cheats Malloori, Jiiva threatens to turn a witness against Sharath and makes him settle the amount to Malloori.
On the other hand, police officer Gopinath is in search of witnesses to shoot Sharath in an encounter. Fearing that Jiiva would help the police, Sharath decides to kill him. What happens after that and whether Jiiva succeeds in his love is narrated in the second half of the movie.
Actor Jiiva, looking handsome in this film, has played the role of a local thug named Blade. The action scenes that are taken with Jiiva keeping a blade in his mouth and spits it into pieces on his enemies have come out perfect. On the whole, he has registered a good performance not only in action sequences but also in romance and sentiment scenes.
Nayanthara, who has taken up a village girl character after a long gap, makes her fans happy with her innocent and homely looks. Picturing a rural get up, the tattoos on her back could have been concealed.
Lohitashwa looks terrific in his evil attitude. Joe Malloori registers himself as a responsible father. TV popular Gopinath, who makes his presence in few shots, is not able to make any impression as a police officer. The comedies of Muniskanth and Karunas are enjoyable.
P.S.Ramnath has taken a story that has a equal mixture of action and romance. Although the story knot falls decades back, choice of the lead cast patches it up with the present.
The music melodies from Srikanth Deva makes the audience enjoy the songs. Even the background music is effective and gives a hope for his good fortunes. Mahesh Muthusamy's cinematography is an added support to the movie.
Totally, Thirunaal is a celebration.


text:
export DYLD_FRAMEWORK_PATH=$BUILT_PRODUCTS_DIR
export DYLD_LIBRARY_PATH=$BUILT_PRODUCTS_DIR

# Create some executables.
test_executables=("$BUILT_PRODUCTS_DIR/gtest_unittest-framework"
                  "$BUILT_PRODUCTS_DIR/gtest_unittest"
                  "$BUILT_PRODUCTS_DIR/sample1_unittest-framework"
                  "$BUILT_PRODUCTS_DIR/sample1_unittest-static")

# Now execute each one in turn keeping track of how many succeeded and failed.
succeeded=0
failed=0
failed_list=()
for test in ${test_executables[*]}; do
  "$test"
  result=$?
  if [ $result -eq 0 ]; then
    succeeded=$(( $succeeded + 1 ))
  else
    failed=$(( failed + 1 ))
    failed_list="$failed_list $test"
  fi
done

# Report the successes and failures to the console.
echo "Tests complete with $succeeded successes and $failed failures."
if [ $failed -ne 0 ]; then
  echo "The following tests failed:"
  echo $failed_list
fi
exit $failed

redpajama_set_name: RedPajamaGithub


A panel of experts have listed off the top five most addictive substances in the world. And several of these substances are legal. What are they and how can they affect your life?
This list was created by chemists, psychiatrists and pharmacologists. Of the top five addictive drugs they ranked, the first on their list is heroin. Animal research has shown this opiate can increase dopamine levels in the brain by up to 200%. Heroin use has risen sharply here in the US, and unfortunately, so has heroin-related overdose deaths.
Next on the list is cocaine. This drug also affects dopamine levels by preventing the brain from turning off the signal. And animal research found cocaine can raise levels to more than 3 times the normal rate.
Third on this list is nicotine. It's found naturally in tobacco and here in the US, more people are addicted to nicotine than any other drug. Which is unfortunate as tobacco smoke has over 7,000 chemicals, and roughly 70 of them can cause cancer.
Number four on the list are barbiturates, otherwise known as "downers". This class of drugs can cause euphoria and high doses can suppress breathing which can be deadly.
And the last drug may surprise you. And that's alcohol. Animal research has shown alcohol can raise dopamine levels in the brain anywhere between 40% and 360%. And the more that was drank, the higher the dopamine level.
Get help for mental health concerns like depression, anxiety or PTSD. Because drug abuse often goes hand in hand with these disorders as many use drugs as a way to cope. Learn how to handle the pressures of life. Please don't use drugs as a way to unwind or ease stress. It's best to avoid all illicit drugs. And be careful not to misuse or abuse prescription drugs. And lastly, if you have teenagers, talk to them openly and honestly about drugs. Communication is essential when it comes to prevention.


text:
College basketball odds and lines
#23 Seton Hall vs. Rutgers: Live stream info, game preview, picks and predictions & more
Rutgers is coming off an exhilarating, buzzer-beating upset of the No. 1 team in the nation. It'll look to carry that momentum into an in-state showdown against No. 23 Seton Hall.
By Nick Simon@Nick_JSimon Dec 12, 2021, 4:25am PST
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Catalina Fragoso-USA TODAY Sports
We'll have an in-state rivalry showdown in New Jersey on Sunday as the Rutgers Scarlet Knights will look for a second straight Top 25 upset when meeting the No. 23 Seton Hall Pirates at the Prudential Center in Newark.
The college basketball world is still buzzing over Rutgers (5-4, 1-1 Big Ten) knocking off No. 1 Purdue 70-68 on Thursday by way of a buzzer beater. Following a Boilermakers layup that put his team down by one with less than four seconds left in the contest, Ron Harper Jr. frantically dribbled up the court and heaved a halfcourt shot that connected as time expired, sending the crowd in Piscataway into a frenzy. It was the perfect way to end a strong night where he put up 30 points and 10 rebounds in the upset.
Seton Hall (8-1) is obviously trying to avoid the same fate as Purdue and is hoping to extend its winning streak to six. The Pirates were also in action on Thursday when it edged Texas at home for a 64-60 victory. Jared Rhoden led with 18 points in the win.
How to watch Seton Hall vs. Rutgers
When: Sunday, December 12th, 7:30 p.m. ET
Where: Prudential Center, Newark, NJ
TV: FS1
Where to live stream online: FOX Sports, FOX Sports App
Live updates and stats: At DraftKings Sportsbook
Spread: Seton Hall -9.5
Total: 135.5
Rutgers +9.5
Rutgers is riding a high off taking down the No. 1 team in the country and the team should get a boost from playing in Newark against a ranked in-state rival. Three of the Scarlet Knights' losses have come within a single score, so they're used to playing in tight contests. They may not win, but they'll give the Pirates a run for their money.


text:
"Practicing is a way of thanking God for our talent. Playing on a Steinway is then a two-way conversations..."
Ádám György
Adam Gyorgy achieved worldwide recognition when he performed at the opening ceremony of EURO 2012, the UEFA European Football Championship in Warsaw, where his unique interpretation of Chopin's Winterwind was televised to 300 million people across the globe.
Through his extraordinary talent and memorable performances, Adam Gyorgy exemplifies the attributes and objectives of the fine arts. As a pianist, he preserves the tradition of historic classical artists. Most well-known for the authenticity of his Liszt interpretations, Adam Gyorgy is recognized as a Liszt ambassador in his home country, Hungary. His recitals have been described by the world's press as 'sensitive', 'playful', 'elegant' and 'warm'. He is also innovative when interpreting classical works with his own distinct and creative style, and creates original music with his improvisations. Adam Gyorgy's captivating personality has won him a loyal international fan base.
Bringing an unprecedented modern twist to classical piano performance, Adam Gyorgy filmed one of his music videos, A Day in New York, in the monumental New York Grand Central Terminal. His performance attracted observers in the busy terminal and created an unexpected pause in the hectic pace of New York City in 2013. He is a regular performer at New York's Carnegie Hall and tours extensively around the world to his global fan base. He is a proud ambassador of Steinway & Sons.
Photo: Maurce Lacroix


text:
package com.tum.ident.fastdtw.timeseries;

import java.util.Random;

/**
 * This class...
 *
 * @author Stan Salvador, stansalvador@hotmail.com
 * @version last changed: Jun 30, 2004
 * @see
 * @since Jun 30, 2004
 */

public class SineWave extends TimeSeries {
	final private static Random rand = new Random();

	// CONSTRUCTORS
	public SineWave(int length, double cycles, double noise) {
		super(1); // 1 dimensional TimeSeries

		// final Random rand = new Random();

		for (int x = 0; x < length; x++) {
			final double nextPoint = Math.sin((double) x / length * 2.0
					* Math.PI * cycles)
					+ rand.nextGaussian() * noise;
			super.addLast(x, new TimeSeriesPoint(new double[] { nextPoint }));
		}
	}

	// PUBLIC FUNCTIONS

} // end class SineWave


text:
Nevada basket maker Datsolalee subject of lecture
April 10, 2018 | Category: News & Events, Press Release
CARSON CITY, Nevada – Like other masters of the arts world, the creations of the famous Native American basket maker Datsolalee, are timeless.
Ninety-three years after her death in Carson City, Datsolalee is widely regarded as one of the most innovative, important and famous basket makers in the world. Her baskets remain coveted by collectors and can be found in top museums throughout the country, including the Smithsonian in Washington, D.C., the Nevada State Museum and Nevada Historical Society.
Her work – much of it done in Carson City and at Lake Tahoe – helped feed the Arts & Craft movement and "Basket Craze" of the early 20th century. At the time, her baskets could sell at up to $2,000. Today, some have been appraised at more than $1 million.
Also known as Louisa Keyser, Datsolalee is the subject of the April Frances Humphrey Lecture Series at the Nevada State Museum, Carson City.
Sue Ann Monteleone, the registrar at the Nevada State Museum who has spent more than 20 years researching the museum's basket collection and Datsolalee, will present the program: "Datsolalee: A Washoe Woman's Legacy to Nevada."
The event is April 26 at 6:30 p.m. at the Nevada State Museum, 600 N. Carson St. The cost is $8 for adults; free for museum members and children 17 and younger.
Monteleone will discuss her research through historic documents, photographs and the study of Datsolalee's baskets.
Monteleone has been the registrar of the Nevada State Museum for 18 years. She has a great passion for basketry and textiles, has studied native plants used for textiles, taken and taught numerous basketry classes with Native American and non-native weavers and is herself a proficient weaver.
Seating for the program is limited and reservations are urged. Those wishing to attend can reserve their seats by registering at www.nvculture.org/nevadastatemuseumcarsoncity/ in the "Upcoming Events" category.


The EU-funded project, PanCareFollowUp (pancarefollowup.eu) looks at how to best deliver survivorship care to survivors of childhood and adolescent cancer in Europe. Survival rates have improved over the last few decades but there is still a long way to go in long-term follow-up care for survivors of childhood cancer.
The aim of PanCareFollowUp is to deliver care according to recently developed guidelines using an innovative model for person centred care that empowers survivors and supports self-management.
The kick-off meeting of 15 January 2019 in Amsterdam enabled the 14 partners from 10 European countries to have a shared and clear vision of their role. All partners reiterated their commitment to delivering the best survivorship care to survivors of childhood and adolescent cancer in Europe.
SIOP Europe's role in PanCareFollowUp includes the coordination of the Survivorship Passport Work Package, as well as communication and dissemination activities in collaboration with the PanCare network and Childhood Cancer International Europe.
This project has received funding from the European Union's Horizon 2020 research and innovation programme under grant agreement No 824982. The material presented and views expressed here are the responsibility of the author(s) only. The EU Commission takes no responsibility for any use made of the information set out.