An electron and a positron undergo pair annihilation (Eq. 44-5). If they had approximately zero kinetic energy before the annihilation, what is the wavelength of eachγproduced by the annihilation?

Short Answer

Expert verified

The wavelength of eachγproduced is 2.43 pm

Step by step solution

01

Concept used to solve the question. 

Annihilation.

When a particle joins its antiparticle, the two of them can annihilate each other. The particle and antiparticle disappear, and their combined energies reappear in some other forms, which are equally shared by the two protons.

If the electron and positron are stationary when annihilating, then their totalenergy is their total mass energy.

02

Find the wavelength of each produced by the annihilation.  

The Annihilation of electron and proton can be given as

e-+e+=γ+γ

We know that the rest energy of the electron,

E=mec2=0.511MeV

Since the mass of both particles is the same, they have the same rest or mass energy.

The total rest energy of the electron-positron pair is

2E=20.511MeV

Therefore, the energy of each γ produced

2Eγ=2E=20.511MeVEγ=0.511MeV

We know that wavelength can be given as

λ=hcE

Where E is energy, c is the velocity of light, h is the plank constant, And the standard value of hc = 1240 eV .nm

Now substituting all the values in the formula

λ=hcEγ=1240eV.nm0.511×10-6eV=2.43×10-3nm=2.43pm

Therefore, the wavelength of eachγproduced is 2.43 pm.

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Most popular questions from this chapter

Question: An electron cannot decay into two neutrinos. Which of the following conservation laws would be violated if it did: (a) energy, (b) angular momentum, (c) charge, (d) lepton number, (e) linear momentum, (f) baryon number?

A particle game.Figure 44-13 is a sketch of the tracks made by particles in a fictionalcloud chamber experiment (with a uniform magnetic field directed perpendicular to the page), and Table 44-6 gives fictionalquantum numbers associated with the particles making the tracks. Particle A entered the chamber at the lower left, leaving track and decaying into three particles. Then the particle creating track 1 decayed into three other particles, and the particle creating track 6 decayed into two other particles, one of which was electrically uncharged—the path of that uncharged particle is represented by the dashed straight line because, being electrically neutral, it would not actually leave a track in a cloud chamber. The particle that created track is known to have a seriousness quantum number of zero.

By conserving the fictional quantum numbers at each decay point and by noting the directions of curvature of the tracks, identify which particle goes with track (a) 1, (b) 2, (c) 3, (d) 4, (e) 5, (f) 6, (g) 7, (h) 8, and (i) 9. One of the listed particles is not formed; the others appear only once each.

Particle

Charge

Whimsy

Seriousness

Cuteness

A

1

1

-2

-2

B

0

4

3

0

C

1

2

-3

-1

D

-1

-1

0

1

E

-1

0

-4

-2

F

1

0

0

0

G

-1

-1

1

-1

H

3

3

1

0

I

0

6

4

6

J

1

-6

-4

-6

Which hadron in Tables 44-3 and 44-4 corresponds to the quark bundles (a) ssu and (b) the dds?

(a) A stationary particle 1 decays into particles 2 and 3, which move off with equal but oppositely directed momenta. Show that the kinetic energy K2 of particle 2 is given by

K2=12E2[E1-E22-E32]

Where, E1,E2,and E3are the rest energies of the particles.

(b) A stationary positive point π+(rest energy 139.6 MeV) can decay to an antimuon μ+(rest energy 105.7 MeV) and a neutrino

ν(rest energy approximately 0). What is the resulting kinetic energy of the antimuon?

Because the apparent recessional speeds of galaxies and quasars at great distances are close to the speed of light, the relativistic Doppler shift formula (Eq.37-31) must be used. The shift is reported as fractional red shift z=Δλλ0

(a)Show that, in termsof,zthe recessional speedparameterβ=vcisgiven by

β=z2+2zz2+2z+2.

(b) A quasar in 1987 has z=4.43. Calculate its speed parameter.

(c) Find the distance to the quasar, assuming that Hubble’s law is valid to these distances.

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