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[QUE/QM-06003] --- Average valueNode id: 1976page For a particle moving in spherically symmetric potential $$V(r) = -V_0 \exp(-r/r_0)$$ and having the wave function $$\psi(r) = N \exp(-\alpha r/r_0) $$ show that $$\langle \mbox{ K.E. } \rangle = {\hbar^2\alpha^2\over 2mr_0^2} ; \qquad \langle\,V(r)\,\rangle = -{8V_0 \alpha^3\over (2\alpha +1)^3}$$ |
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[QUE/QM-06001] --- Average value Node id: 1977page Let $$ \chi(x)= \exp(ik_0x)\psi(x) .$$ Show that $$\langle \hat{p} \rangle_\chi = \hbar k_0 + \langle\hat{p} \rangle_\psi $$
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[QUE/QM-06002] Average value Node id: 1978page For a particle having the wave function $$\psi(x) = N \exp(-x^2/\alpha^2)$$ compute the averages of the following dynamical variables. (a) kinetic energy, (b) $V_1(x) = V_0 |x|^{2m+1}$ (c) $V_2(x) =kx^2$ |
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[QUE/QM-06005]Node id: 1993pageA particle has the wave function $$ \psi(x)= A\exp(-|x|/\alpha) .$$ compute the following quantities.
- Find the probability that the momentum will lie between $p$ and $p=\Delta p$.
- Compute the uncertainties $\Delta x$ and $\Delta p$.
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[QUE/QM-06006]Node id: 1994pageFor a harmonic oscillator in the ground state find the average values of kinetic energy, potential energy and $|x|^{2m+1}.$ |
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[QUE/QM-06007]Node id: 1995pageFor the ground state and the first excited state of H-atom find the value of $r$ for which the probability density is maximum. |
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[QUE/QM-06011]Node id: 1999pageGiven that :The vector space needed to describe a particular physical system is two dimensional complex vector space. The states are therefore represented by 2 component complex column vectors. The observables for this system are $2\times2$ matrices. A set of three dynamical variables of the system, $X,Y,Z,$ are be represented by $2\times 2$ matrices denoted by $\sigma_x, \sigma_y,\sigma_z$, where $$ \sigma_x =\begin{pmatrix}0&1\\1&0\end{pmatrix},\qquad \sigma_y=\begin{pmatrix}0&-i\\i&0\end{pmatrix}, \qquad \sigma_z=\begin{pmatrix}1&0\\0&-1\end{pmatrix}.$$ Answer the following question %----------------------------------------------------------------------------- Question : What vector would represent the state of the system if it is known that the system has definite value $+1$ for the dynamical variable $X$? What vector would represent the state if the system has definite value $-1$ for the variable $Y$. |
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[QUE/QM-06008]Node id: 1996pageFor the value of $r$ for which the position probability density is maximum for the electron in the $n^{th}$ excited state. How does this maximum shift when $n$ is increased? |
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[QUE/QM-06010]Node id: 1998page The vector space needed to describe a particular physical system is two dimensional complex vector space. The states are therefore represented by 2 component complex column vectors. The observables for this system are $2\times2$ matrices. A set of three dynamical variables of the system, $X,Y,Z,$ are be represented by $2\times 2$ matrices denoted by $\sigma_x, \sigma_y,\sigma_z$, where $$ \sigma_x =\begin{pmatrix}0&1\\1&0\end{pmatrix},\qquad \sigma_y=\begin{pmatrix} 0&-i\\i&0\end{pmatrix}, \qquad \sigma_z=\begin{pmatrix}1&0\\0&-1\end{pmatrix}.$$ What values are experimentally allowed if one measures the dynamical variable
- $X$
- $Z$
- $T= X^2+Y^2+Z^2$
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[QUE/QM-06012] Node id: 2000pageThe vector space needed to describe a particular physical system is two dimensional complex vector space. The states are therefore represented by 2 component complex column vectors. The observables for this system are $2\times2$ matrices. A set of three dynamical variables of the system, $X,Y,Z,$ are be represented by $2\times 2$ matrices denoted by $\sigma_x, \sigma_y,\sigma_z$, where $$ \sigma_x =\begin{pmatrix}0&1\\1&0\end{pmatrix},\qquad \sigma_y=\begin{pmatrix}0&-i\\i&0\end{pmatrix}, \qquad \sigma_z=\begin{pmatrix}1&0\\0&-1\end{pmatrix}.$$ Show that the allowed values of $$ X_{\hat{n}} = n_1 X + n_2 Y + n_3 Z $$ are given by $\pm \sqrt{n_1^2+n_2^2+n_3^2}.$ |
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[QUE/QM-06013]Node id: 2001pageThe vector space needed to describe a particular physical system is two dimensional complex vector space. The states are therefore represented by 2 component complex column vectors. The observables for this system are $2\times2$ matrices. A set of three dynamical variables of the system, $X,Y,Z,$ are be represented by $2\times 2$ matrices denoted by $\sigma_x, \sigma_y,\sigma_z$, where $$ \sigma_x =\begin{pmatrix}0&1\\1&0\end{pmatrix},\qquad \sigma_y=\begin{pmatrix}0&-i\\i&0\end{pmatrix}, \qquad \sigma_z=\begin{pmatrix}1&0\\0&-1\end{pmatrix}.$$ If the state vector of the system is given by $$ \left( \begin{array}{r} \displaystyle{1\over\sqrt{5}}\\[4mm] \displaystyle {-2\over\sqrt{5}} \end{array} \right) $$ Find the probability that
- a measurement of $X$ will give value $1$.
- a measurement of $Y$ will give value $-1$.
- a measurement of $Z$ will give value $1$.
- a measurement of $X+Y$ will give value $\sqrt{2}$.
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[QUE/QM-06014]Node id: 2002page\(\newcommand{\ket}[1]{|#1\rangle}\) Compute the uncertainty, \(\Delta E\), in energy is a state \[ \ket{\psi}= \alpha_1 \ket{E_1} + \alpha_2\ket{E_2}. \] Show that the uncertainty vanishes when \(E_1=E_2\). Is this result expected? WHY?
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[QUE/QM-06017]Node id: 2004pageThe vector space needed to describe a particular physical system is two dimensional complex vector space. The states are therefore represented by 2 component complex column vectors. The observables for this system are $2\times2$ matrices. A set of three dynamical variables of the system, $X,Y,Z,$ are be represented by $2\times 2$ matrices denoted by $\sigma_x, \sigma_y,\sigma_z$, where $$ \sigma_x =\begin{pmatrix}0&1\\1&0\end{pmatrix},\qquad \sigma_y=\begin{pmatrix}0&-i\\i&0\end{pmatrix}, \qquad \sigma_z=\begin{pmatrix}1&0\\0&-1\end{pmatrix}.$$ State which of the following operators can represent an observable quantity and which ones cannot represent an observable.
- $X_P = X+iY$
- $X_M=X-iY$
- $R=3X + 12Y + 4Z$
- $T= X^2+Y^2+Z^2$
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[QUE/QM-06108]Node id: 2005page A particular state of a physical system is represented by \[\psi = \begin{pmatrix} 1 \\ 1+i \\ 1-i \end{pmatrix}.\] Find value of \(\lambda\) such that the vector \(\phi\), where \[ \phi= \begin{pmatrix} \lambda \\ 2i \\ 2\end{pmatrix}\] may represent the same state as \(\psi\). \paragraph*{Answer: \(\lambda = (1+i)\)} |
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[QUE/QM-06019]Node id: 2006pageUsing spectral theorem, or otherwise, show that \begin{equation} \exp(i\hat{P}a) (\hat{x})^n \exp(-i\hat{P}a ) = (\hat{x}+a)^n, \end{equation} where \(n\) is an integer and \(\hat{P}\) and \(\hat{x}\) are the momentum and position operators. |
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[QUE/QM-06020]Node id: 2007pageFind the adjoint of an operator \(S\), defined on the space of square integrable functions, given below. \begin{equation*} Sf(x) = \alpha f(2x) \end{equation*} find a value of \(\alpha\) so that \(S\) may be unitary. Is the value you found unique? |
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[QUE/QM-06021]Node id: 2008pageA dynamical variable \(S\) of a system is represented by a \(3\times3\) matrix: \begin{eqnarray} S= \begin{pmatrix} 0 & 1 & 0\\ 1 & 0 & 1\\ 0&1&0 \end{pmatrix}. \end{eqnarray}
- Find all allowed values of \(S\). If the state of a system is given by the vector \[ f= \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} \]
- Compute the probability of getting possible different values when a measurement of \(S\) is made.
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[QUE/QM-06023]Node id: 2011page Apply first postulate of quantum mechanics and for each of the of the following wave functions which ones represent wave functions the same state as \(\psi(x,t)\)? and which ones represent a different state?
- \(\exp(\Lambda(x)) \psi(x)\)
- \(\exp(i\Lambda(x)) \psi(x)\)
- \(\exp(i\alpha) \psi(x)\)
- \(\exp(\alpha) \psi(x)\)
where \(\Lambda(x)\) is a real function of \(x\) and \(\alpha\) is a real constant.
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[QUE/QM-06024]Node id: 2012pageIf \(\psi(x,y,z)\)is the wave function of a particle in three dimension write expression for probability that
- \(x\) is between \(x_1\) and \(x_2\);
- \(p_z\) lies between \(p_1\) and \(p_2\);
- Assume that \(\psi(\vec{r}) = R(r) Y_{\ell m}(\theta,\phi)\). What is the probability that the particle will be found inside a sphere of radius \(R\)? What is the probability that the particle will be found outside the sphere of radius \(R\)?
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[QUE/QM-06025]Node id: 2013pageDefine uncertainties in position and momentum and compute their values for the wave packet with wave function \[ \psi(x) = \frac{a}{\surd \pi} e^{-x^2/2a^2}\] |
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