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[QUE/EPP-01010]Node id: 2635pageThe decay of a massive particle \(A\) into two particles \(B,C\) \begin{equation} A \longrightarrow B + C \end{equation} is not possible when \(M_A < M_B + M_C\).
- Show this by applying momentum energy conservation in the rest frame of particle \(A\).
- Why does your argument not remain valid for the case when mass of particle \(A\) goes to zero.
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[QUE/EPP-01009]Node id: 2634pageUse uncertainty relation to estimate the potential needed to confine an electron inside a nucleus, Take the size of nucleus to be \( R \approx 10^{-12}\) cm. |
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[QUE/EPP-01008]Node id: 2633page The values of \(mc^2\) for the pion \(\pi^+\) and muon \(\mu^+\) are 139.57MeV and 105.66 MeV respectively. Find the kinetic energy of the muon decay in \[ \pi^+ \longrightarrow \mu^+ + \nu_\mu \] assuming that the neutrino is massless. For a neutrino of finite but very small mass \(m_\nu\) show that, compared with the case of a massless neutrino, the muon momentum would be reduced by the fraction \begin{equation*} \frac{\Delta p}{p} = - \frac{m_\nu^2(m_\pi^2+m_\mu^2)}{(m_\pi^2-m_\mu^2)^2} ~\text{MeV} \approx -\frac{m_\nu^2}{10^4}. \end{equation*} where \(m_\nu\) is neutrino mass in MeV. |
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[QUE/EPP-01007]Node id: 2632pageFor a two particle reaction \[ A + B \longrightarrow C + D\] define variables \(s,t,u\) by \begin{equation} s= (p_1+p_2)^2; \quad t= (p_1-p_3)^2; \quad u = (p_1-p_4)^2, \end{equation} where \(p_1, p_2,p_3,p_4\) denote the four momenta of the particles \(A,B,C\) and \(D\).
- Show that \[ s+ t + u = \sum_{k=1}^4 m_k^2\] where \(m_k, k=1,..,4\) are the masses of the four particles in the reaction.
- Find the allowed range of variables \(t\) and \(u\) in terms of the masses of the particles.
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[QUE/EPP-01032]Node id: 2671pageAn analysis of measurement of position, the famous Heisenberg microscope thought experiment, leads to uncertainty relation with momentum uncertainty identified with the momentum transfer. Using similar idea show that the distance probed in a scattering experiment \[ A + B \longrightarrow A + B\] is approximately \(1/\sqrt{t}\), where $t=(p_A-q_A)^2\), where \(p_A, p_B\) denote the initial and \(q_A, q_B\) denote the final four momenta of the two particles.
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[QUE/EPP-01030]Node id: 2668page
- Alpha particles of energy 7 MeV are incident from a gold foil in a scattering experiment.
- Plot the electrostatic potential seen by the alpha particlesFind the closest distance an alpha particle can reach to the nucleus assuming that initially the alpha particle was on a direct collision course with the gold nucleus.
How will your answers change if the positive charge of the gold nucleus is assumed to be uniformly distributed over a sphere of radius of a few Angstroms, as was proposed in Thompson model? |
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[QUE/EPP-01031]Node id: 2670pageFind the charge \(Q\) that will exert the same force on an electron at 1 nm as the Sun's gravitational pull on the Earth. |
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[SHQ/QM-06002] --- Allowed outcomes of measurement Node id: 1965page |
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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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22-04-17 21:04:52 |
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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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22-04-17 21:04:07 |
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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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