If the probability that x lies between x and x + dx is P(x) dx = ae-ax dx, where 0 < x < ∞ , a > 0, then the probability that x lies between x1 and x2 (x2 > x1) is
A Michelson interferometer is illuminated with monochromatic light. When one of the mirrors is moved through a distance of 25.3 μm, 92 fringes pass through the cross-wire. The wavelength of the monochromatic light is
An electron is in a statewith spin wavefunction {\phi _s} = \left[ {\begin{array}{*{20}{c}}
{\frac{{\sqrt 3 }}{2}} \\
{\frac{1}{2}}
\end{array}} \right] in the sz representation. What is the probability
of, finding the z-component of its spin along the −Z^ direction?
If the wave function of a particle trapped in space between x = 0 and x = L is given by ψ(x)=Asin(L2πx), where A is a constant, for which value(s) of x will the probability of finding the particle be the maximum?
The normalized eigen states of a particle in a one-dimensional potential well V\left( x \right) = \left\{ {\begin{array}{*{20}{c}}
{0,}&{{\text{if }}0 \leqslant x \leqslant a} \\
{\infty ,}&{{\text{otherwise}}}
\end{array}} \right. are given by ψn(x)=a2sin(anπx) where, n = 1, 2, 3, . . .
The particle is subjected to a perturbation V′x=V0cos(aπx),for 0⩽x⩽2a=0,otherwise
The shift in the ground state energy due to the perturbation, in the first order perturbation theory, is
A parallel beam of electrons of a given momentum pass through a screen S1 containing a slit and then produces a diffraction pattern on a screen S2 placed behind it. The width of the central maximum observed on the screen S2 can be increased by
An exact measurement of the position of a Simple Harmonic Oscillator (SHO) is made with the result x = x0, [The SHO has energy levels En (n = 0, 1,
2, . . .) and associated normalized wave functions ψn ]. Subsequently, an exact measurement of energy E is made, using the general notation Pr(E = E') denoting the probability that a result E' is obtained for this measurement, the following statements are written. Which one of the following statements is correct?
An atomic state of hydrogen is represented by following wave function ψ(r,θ,ϕ)=21(a01)23(1−2a0r)e2a0−rcosθ where, a0 is a constant. The quantum numbers of the state are
The expectation value of the z coordinate, (z), in the ground state of the hydrogen atom (wave function: ψ100(r)=Ae−a0r, where A is the normalization constant and a0 is the Bohr radius), is
The spin' function of a free particle, in the basis in which sz is diagonal can be written as \left[ {\begin{array}{*{20}{c}}
1 \\
0
\end{array}} \right] and \left[ {\begin{array}{*{20}{c}}
0 \\
1
\end{array}} \right] with eigen values +2ℏ and −2ℏ respectively. In the given basis, the normalized eigen function of sy with eigen value −2ℏ is
A one-dimensional harmonic oscillator is in the state ψ(x)=141[3ψ0(x)−2ψ1(x)+ψ2(x)], where, ψ0(x),ψ1(x) and ψ2(x) are the ground, first excited and second excited states, respectively. The probability of finding the oscillator in the ground state is
Let L = (Lx, Ly, Lz) denotes the orbital angular momentum operators of a particle and let L+ = Lx + i Ly and L- = Lx - i Ly. The particle is in aneigen state of L2 and Lz eigen values ℏ2(l+1) and ℏl respectively. The expectation value of L+L- in this state is
A one-dimensional harmonic oscillator carrying a charge -q is placed in a uniform electric field E along the positive X-axis. The corresponding Hamiltonian operator is
An electron propagating along the X-axis passes through a slit of width ∆y = 1 nm. The uncertainty in the y-component of its velocity after passing through the slit is