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Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18....

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Main points of today’s lecture: Direct Reactions: Summary – Resonances Compound nucleus Relativistic kinematics Main points of last lecture: – exam Physics 492 Lecture 17
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Page 1: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

• Main points of today’s lecture:– Direct Reactions: Summary– Resonances – Compound nucleus– Relativistic kinematics

• Main points of last lecture:– exam

Physics 492 Lecture 17

Page 2: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Same technique can be used for inelastic scattering

• Measurement of inelastic scattering on 26Mg

26Mg

Page 3: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

These were examples of “direct reactions”What are properties of direct reactions?

Page 4: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Compound nuclear reactions

• important at low incident energies E<30 MeV

Page 5: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Example of CN reactions

• Inelastic proton scattering on 50Cr

Page 6: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Branching ratios in CN decay

Page 7: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Resonance shape reflects interference with direct background

• Left side shows destructive interference. Right side does not.

Page 8: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Consider simple case p+4He

Page 9: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Breit-Wigner resonance formula

• If there is no direct background and only one decay channel, theresonance scattering amplitude is given by.

Page 10: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Relationship to lifetime

Page 11: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Lifetimes of short lived states

• Two ways to measure lifetime:– Focus on exponential decay law:

– Measure width of state:

Page 12: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Consider simple case p+4He

Page 13: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Resonances with multiple decay channels

• Need to consider Branching Ratios

Page 14: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Summary of Compound nuclear reactions

Page 15: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

• Main points of today’s lecture:– Relativistic transformations– Four vectors– Invarients,

• Proper time• Inner products of vectors

– Momentum– Example: Photon-electron

scattering

• Main points of last lecture:– Compound nucleus– extrance and exit channel– Symmetries and selection rules

Physics 492 Lecture 18

Page 16: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Relativistic Kinematics

• When is it necessary?

• Review: Special relativity is based upon– Laws of Physics are independent of the inertial frame– Speed of light=c in all frames

Page 17: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Lorentz transformations

• Consider two inertial frames S and S’ whose velocities differ by Δvz= vt.

Page 18: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Matrix formulation

• In matrix form

• Inverse transformation

Page 19: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Identity

• If we transform and then transform back, we should get the same 4 vector.

Page 20: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Time dilation

• Consider the transformation of the point at the origin of S’

Page 21: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Inner Products

• What is an inner product?

• What are the properties of an inner product?

Page 22: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

What is the correct 4-vector inner product

• Add time-like component with the opposite sign as the space-like component. Check whether it is an invariant

→It is an invariant!

Page 23: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Formal expressions

• The metric:

Page 24: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Other metrics

• You have used metrics without knowing it

Page 25: Physics 492 Lecture 17 - Michigan State Universitylynch/lecture_wk7.pdf · Physics 492 Lecture 18. Relativistic Kinematics • When is it necessary? • Review: Special relativity

Other 4 vectors

• “4-velocity” and 4-momentum

value for inner product


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