Post on 05-Jan-2016
description
Quantum Noise in (High-Gain) FELs
Kwang-Je Kim
Argonne National Laboratory
March 8, 2012
Future Light Sources WS
Jefferson Laboratory
Newport News, VA
Quantum Noise KJK FLS 2012
2
EM Field Operator Complex field amplitude operator ( Hermitian conjugate)
Intensity = ,
=(annihilation, creation operator)
=1, = number operator from vacuum fluctuation
Quantum Noise KJK FLS 2012
3
Linear amplifier =(input, output) field operator ; =amplitude gain operator for gain medium;
= | =+; 2 =power gain
In the absence of initial photons; Can show The minimum noise is ½ input photon from VF and ½
input photon from amplifier reaction Low noise in gain device (oscillator)
Quantum Noise KJK FLS 2012
4
Proof (C. M. Caves, PRD, 1817 (1982))
: Condition for minimum noise: =0
Quantum Noise KJK FLS 2012
5
FEL equation Classical : Field energy density Quantum:=1 :
, ;
Quantum Noise KJK FLS 2012
6
Heisenberg FEL equation in collective variables (R. Bonifacio, et.,al.) Bunching factor Collective momentum Assume . =classical, and small
, , Formally identical to classical equation
Quantum Noise KJK FLS 2012
7
Solution exp(ilt) , maximum growth
;
Quantum Noise KJK FLS 2012
8
Amplified power
The first two terms are classical coherent amplification and SASE, respectively
Random electron distribution Noise suppression schemes ( A. Gover,..)
Classical (KJK and RRL, FEL 2011) and quantum
limitation of the suppression
Quantum Noise KJK FLS 2012
9
Quantum noise ; representation Assume Gaussian wavefunction
Cross terms do not contribute
(C. Schroder, C. Pellegrini, P.Chen) Minimum =3/2 However the minimum should be 1=1/2+1/2
Quantum Noise KJK FLS 2012
10
Minimum noise wavepacket Require:
: minimum noise To understand phase space distribution, look at Wigner function
Tilted phase space, or chirped
Quantum Noise KJK FLS 2012
11
Magnitude of minimum quantum noise relative Random SASE
Small but not negligible