Kinematics variables.pdfrelativistic kinematics reaction kinematics

Nuclear Reactions
Some Basics
II. Reaction Kinematics

Reaction Kinematics
• A beam incident on a target will result in many different reactions,
including elastic and inelastic scattering, representing different collisions
of beam particles with different nuclei.
• To isolate a specific reaction (to measure, e.g., its cross section or some
other prediction of theory), in addition to identifying the correct particles
involved, we need to “look” at the right place, i.e. isolate products moving
in the “correct” momentum (i.e. energy and direction).
• To assist in identifying the correct energy and direction of emitted
particles, we utilize the kinematics of the reaction, i.e. the predictions of:
– Conservation of energy
– Conservation of linear momentum
for this reaction (for CEBAF energies, must use relativistic expressions)
• Two-body kinematics
– Used when two particles are present in the “final state” (i.e. after collision)
• Three-body kinematics
– Used when three particles are present in the final state

Two-Body Kinematics
Elastic Scattering in a plane (non-relativistic)
p1
K1
m2
m1
K1’
P2’
K2’
θ1’
m2
P1’
m1
θ2’
Given initial state: m1, m2, p1, p2=0
Find final state: K1’, K2’, θ2’, θ2’
• Recall: K = ½ mv2, p = mv, K = p2/2m
• Only relevant physics laws are conservation of energy and momentum
• Conservation of Energy: K1 = K1’ + K2’ (1)
• Conservation of Momentum: p1 = p1’cosθ1’ + p2’cosθ2’ (2)
0 = p1’sinθ1’ - p2’sinθ2’ (3)
• We have 3 equations, and 4 unknowns (K1’,K2’, θ1’ ,θ2’)
• Therefore K’s and θ’s are not uniquely determined
• If given one of the final state variables we can calculate the other three

Two-Body Kinematics
Elastic Scattering in a plane (non-relativistic)
Some Observations
• If the initial conditions (m1, m2, , =0) are known in an actual elastic
scattering experiment, and if a final state particle is chosen to be detected at an
angle θ1, two-body kinematics determine a unique angle θ2 at which the other
particle will emerge as well as both kinetic energies.
• Said differently, if two detectors are to detect particles corresponding to a single
elastic scattering event, they have to be placed at “conjugate” angles, i.e.
angles related through two-body kinematics
• Note: A single elastic scattering event (labeled A) detected at conjugate angles
(θ1, θ2)A is represented by a single point on a plot of K1’ vs. K2‘ . For the same
initial conditions, another event with particles detected at a different set of
conjugate angles (θ1, θ2)B will produce a different combination of K1’ and K2’
and will be represented by a different single point (labeled B) on the same plot.
1
p
r
2
p
r
K2’
K1’
A
B

Two-Body Kinematics
Elastic Scattering (Relativistic)
• Conservation of (total) Energy (here use c =1):
E1 + m2 = E1’ + E2’ (1)
• Conservation of Momentum:
p1 = p1’cosθ1’ + p2’cosθ2’(2)
0 = p1’sinθ1’ - p2’sinθ2’ (3)
• Recall: E1 = K1 + m1 and E1
2 = p1
2 +m1
2
E1’ = K1’ + m1 and E1’2 = p1’2 +m1
2
E2’ = K2’ + m2 and E2’2 = p2’2 +m2
2
• Solve (1), (2), (3) for K1’, K2’, θ2’
p1
K1
m2
m1
K1’
P2’
K2’
θ1’
m2
P1’
m1
θ2’
Given: m1, m2, K1, θ1’
Find: K1’, K2’, θ2’

Relativistic Two-Body Kinematics
Elastic Scattering – Results (1)
( ) ( )
[ ]
( )
[ ]
( ) ( )
[ ]
( )
[ ]
( ) ( ) ( )
2
1
'
1
2
2
1
2
2
1
'
1
2
1
'
2
'
2
2
2
1
2
2
1
'
2
2
2
1
2
2
1
2
2
2
2
'
2
1
2
1
2
'
2
'
1
2
2
1
2
2
1
'
1
2
2
1
2
2
1
2
1
2
1
'
1
1
2
1
1
'
1
ρ
1
θ
cot
ρ
1
γ
ρ
ρ
cotθ
ρ
ρ
1
cotθ
θ
cos
p
m
E
2
θ
cos
p
m
E
4m
A
cosθ
p
m
E
A
E
θ
cos
p
m
E
2
θ
cos
p
m
E
4m
A
cosθ
p
m
E
A
E
−
+
−
+
±
+
−
=
−
+
−
+
−
±
+
=
−
+
−
+
−
±
+
=
Where A1, A2, ρ1, ρ2, γ are given by:

Elastic Scattering – Results (2)
( )
( )
( ) ( )
[ ]
( ) ( )
[ ]
( )
2
1
2
2
1
2
1
2
2
cm
2
1
2
2
1
2
2
2
2
2
1
1
2
2
2
1
2
2
1
2
1
2
1
2
1
1
1
1
1
2
2
1
2
2
2
1
2
2
1
2
1
1
m
2E
m
m
m
E
c
v
1
1
γ
p
m
E
4m
A
m
E
p
A
ρ
p
m
E
4m
A
m
E
p
A
ρ
K
m
m
m
m
2
A
K
m
m
m
m
2
A
+
+
+
=
−
=
−
+
−
+
=
−
+
−
+
=
+
+
=
+
+
=
Interactive program that calculate 2-body kinematics:
http://www.calstatela.edu/academic/nuclear_physics/2bdkin.html

Elastic Scattering - Observations
• Note: Not any θ1, θ2 pairs are possible in two-body kinematics
– Square root in E1, E2 must be > 0
• Note: If m1 = m2 then θ1’ + θ2’ < π/2 (unlike classical mechanics)
• Interactive program that calculate 2-body kinematics:
– http://www.calstatela.edu/academic/nuclear_physics/2bdkin.html
( )
[ ]
( )
[ ]
2
1
2
2
1
2
2
2
1
2
2
2
2
'
2
2
2
1
2
1
1
2
2
2
1
2
1
2
1
'
1
2
p
4m
K
2m
m
m
4m
A
θ
sin
p
4m
K
2m
m
m
4m
A
θ
sin
+
+
−
≤
+
+
−
≤

Three-Body Kinematics
Nuclear Reaction (Relativistic)
mT
K1’
P2’
K2’
θ1’
P1’
m1
θ2’
m2
po
Ko
mo
θ3’
mR
PR
KR
• Conservation of energy and momentum hold again.
Eo + mT = E1’ + E2’ + ER’ (1)
po = p1’cosθ1’ + p2’cosθ2’ + pRcosθ3’ (2)
0 = p1’sinθ1’ - p2’sinθ2’ + pRsinθ3’ (3)
– In addition, but ignore for now, there may be “out-of-plane” (φ) momentum
components
• Here we have 3 equations and 6 unknowns (E1’, E2’, ER’, θ1’, θ2’, θ3’)
• Need to know 3 variables in the final state to compute everything else

Computing
Relativistic Three-Body Kinematics
• Will not solve analytically expressions for unknowns here.
• Go to:
http://www.calstatela.edu/academic/nuclear_physics/kin3
b.htm
– On-line program that computes relativistic three-body kinematics

Relativistic Three-Body Kinematics
Nuclear Reaction – An Observation
• If 2 of the 3 final state unknowns are specified (e.g. by specifying
the energy and direction of one of the detected particles) the
reaction is represented on the E1
’ vs E2
’ plot for the remaining 2
particles by a curve (compared to a point in 2-body scattering)
• In computing the 5-fold cross section:
N corresponds to events on the curve projected to “byte”∆E2’
E2’
2'
2'
1'
2'
2'
1'
5
∆E
∆Ω
Qnx∆
Ne
dE
dΩ
dΩ
σ
d
Ω
=
E1’
N
∆E2’

The 3He(e,e’p)2H Reaction Mechanism
• The presumed reaction mechanism is represented by the
diagram:
• This is known as the Plane Wave Impulse Approximation,
i.e. virtual photon interacts only with a single bound proton,
which is subsequently ejected from the target and detected,
while leaving the rest of 3He (i.e. 2H) unaffected (spectator)
• Valid at high energies (e.g. CEBAF)
• Note: Only one virtual photon is assumed to be exchanged
2H
p
p
γ
3He
e
e’

Definitions of Kinematic Variables
• Incident electron: momentum ki, total energy Ei , mass me
• Scattered (and detected) electron: kf, Ef, me
• Ejected (and detected) proton: pp, Ep, mp
• Target nucleus (3He): pA, EA, MA
• Left over nucleus (2H, spectator): pB, EB.
• NOTES (all quantities in lab frame):
– Target momentum pA=0 (target at rest in lab)
– Target total energy EA = mAc2 (target at rest, rest energy only)
– Ei = Ti (kinetic energy of incident electron) + mec2 (its rest energy)
• Here ignore mec2 = 0.511 MeV since Te =1-6 GeV at CEBAF >> mec2
Therefore: Ei ≈ Ti ≈ ki (recall E2 = k2c2 + (moc2)2, E in MeV/c2, k in Mev/c)
– Ef ≈ Tf ≈ kf (similarly)
– (here can’t neglect rest energy, heavier proton is
not ultra-relativistic)
2
2
p
2
2
p
p )
c
(M
c
p
E +
=

Some Additional Kinematic Variables
Scattering plane
(contains e, e’)
Reaction plane
(contains ‘γ’ and p)
Angle between scattering
and reaction planes
• Incident electron scattering angle: θe
• Angle between scattering and reaction planes: φ
– “In-plane” kinematics: φ = 0 (p “forward” of q), φ = π (p “backward” of q)
– “out-of-plane” kinematics: φ ≠ 0
• Angle between q and pp: θpq

Additional Kinematic Variables
• In a typical (e,e’p) experiment we measure:
– Ei, ki (incident beam energy, momentum)
• Recall: Ei = Ti = ki (ultra-relativistic electrons)
– Ef, kf (scattered electron energy, momentum, using Hall A HRS)
• Similarly recall: Ef = Tf = kf (ultra-relativistic electrons)
– pp (momentum of ejected proton (using Hall A HRS)
• Virtual photon momentum q may be calculated from conservation of
momentum at the e-e’-’γ vertex (ki = kf + q):
q = ki – kf
• Virtual photon energy ω may be calculated from conservation of
energy at the same vertex (Ei = Ef + ω):
ω = Ei – Ef
• q and ω are also the momentum and energy transferred to (and
absorbed by) the target nucleus by the virtual photon through this
collision.

Missing Momentum and Energy
• “Missing momentum”, pmiss, is the momentum of the undetected recoil
nucleus (2H). It may be calculated from conservation of momentum at
the ‘γ’-3He-p vertex (q = pp + pB). Therefore:
pmiss ≡ pB = q - pp
• “Missing energy”, Emiss, is the unaccounted part of the energy transfer
ω after kinetic energies Tp and TB of the known pieces of the broken up
nucleus are subtracted from it. i.e.
Emiss = ω – Tp – TB
– Note: Tp = Ep - Mpc2 = (pp
2c2 + Mp
2c4)1/2 – Mpc2
TB = EB – MBc2 = (pB
2c2 + MB
2c4) 1/2 – MBc2
• Note: Since the values of ki, kf, pp, are known (measured), the values of
q, ω, pmiss and Emiss can be calculated for each event of this reaction.

The Emiss Spectrum for 3He(e,e’p)X
• Emiss consists of the energy required to “separate” (un-bind) the
ejected proton from the target nucleus plus any “excitation” energy
the recoil nucleus might have (above its lowest, ground state). i.e.
Emiss = Esep + Eexc
where: Esep = Mpc2 + MBc2 – MAc2
• Since 3He does not have any excited states, and if the only e+3He
reaction channel possible is 3He(e,e’p)2H, there should be only one
peak in the Emiss spectrum, at the value of Esep, which can be
calculated to be 5.49 MeV (from mA = mp + m2H + Esep).
• Of course, there are additional channels available, including the 3-body
breakup channel 3He(e,e’p)pn and particle creation at higher Emiss,
leading to additional features in the Emiss spectrum.
• The 2H nucleus (deuteron) has a binding energy of (i.e. it breaks up at)
2.22 MeV. Therefore a second peak would be expected in the
spectrum at Emiss = 5.49 + 2.22 = 7.71 MeV. See Figure in next slide…

The Emiss Spectrum for 3He(e,e’p)X #1

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