Acceleration voltage

Longitudinal voltage

The longitudinal effective acceleration voltage is given by the kinetic energy gain experienced by a particle with velocity β c along a defined straight path (path integral of the longitudinal Lorentz forces) divided by its charge,

V ∥ ( β ) = 1 q e → s ⋅ ∫ F → L ( s , t ) d s = 1 q e → s ⋅ ∫ F → L ( s , t = s β c ) d s .

For resonant structures, e.g. SRF cavities, this may be expressed as a Fourier integral, because the fields E → , B → , and the resulting Lorentz force F → L , are proportional to exp ⁡ ( i ω t ) (eigenmodes)

V ∥ ( β ) = 1 q e → s ⋅ ∫ F → L ( s ) exp ⁡ ( i ω β c s ) d s = 1 q e → s ⋅ ∫ F → L ( s ) exp ⁡ ( i k β s ) d s with k β = ω β c

Since the particles kinetic energy can only be changed by electric fields, this reduces to

V ∥ ( β ) = ∫ E s ( s ) exp ⁡ ( i k β s ) d s

Particle Phase considerations

Note that by the given definition, V ∥ is a complex quantity. This is advantageous, since the relative phase between particle and the experienced field was fixed in the previous considerations (the particle travelling through s = 0 experienced maximum electric force).

To account for this degree of freedom, an additional phase factor ϕ is included in the eigenmode field definition

E s ( s , t ) = E s ( s ) exp ⁡ ( i ω t + i ϕ )

which leads to a modified expression

V ∥ ( β ) = e i ϕ ∫ E s ( s ) exp ⁡ ( i k β s ) d s

for the voltage. In comparison to the former expression, only a phase factor with unit length occurs. Thus, the absolute value of the complex quantity | V ∥ ( β ) | is independent of the particle-to-eigenmode phase ϕ . It represents the maximum achievable voltage that is experienced by a particle with optimal phase to the applied field, and is the relevant physical quantity.

Transit time factor

A quantity named transit time factor

T ( β ) = | V ∥ | V 0

is often defined which relates the effective acceleration voltage V ∥ ( β ) to the time-independent acceleration voltage

V 0 = ∫ E ( s ) d s .

In this notation, the effective acceleration voltage | V ∥ | is often expressed as V 0 T .

Transverse voltage

In symbolic analogy to the longitudinal voltage, one can define effective voltages in two orthogonal directions x , y that are transversal to the particle trajectory

V x , y = 1 q e → x , y ⋅ ∫ F → L ( s ) exp ⁡ ( i k β s ) d s

which describe the integrated forces that deflect the particle from its design path. Since the modes that deflect particles may have arbitrary polarizations, the transverse effective voltage may be defined using polar notation by

V ⊥ 2 ( β ) = V x 2 + V y 2 , α = arctan ⁡ V ~ y V ~ x

with the polarization angle α The tilde-marked variables are not absolute values, as one might expect, but can have positive or negative sign, to enable a range [ − π / 2 , + π / 2 ] for α . For example, if V ~ x = | V x | is defined, then V ~ y = V y ⋅ exp ⁡ ( − i arg ⁡ V x ) ∈ R must hold.

Note that this transverse voltage does not necessarily relate to a real change in the particles energy, since magnetic fields are also able to deflect particles. Also, this is an approximation for small-angle deflection of the particle, where the particles trajectory through the field can still be approximated by a straight line.