The TM
010 mode of the MCR cavity has the lowest resonant frequency (
) and the longest resonant wavelength (
). TM
010 single-mode operation is often used to accelerate charged particles, and the cavity is called an accelerating cavity [
20], and the mode is called an accelerating mode. Now we begin to discuss the microwave photon structures of the TM
010 mode in the MCR cavity, and compare it with the mathematical description of the classical EM field.
4.1. The EM Field of the TM010 Mode in a MCR Cavity
In the MCR cavity with inner radius
R and length
L, the exact expressions of the EM field distribution of all resonant modes in the cavity are given in classical electrodynamics [
21,
22]. The EM field distribution of the TM
010 mode is the simplest, as follows:
The TM
010 mode is an accelerating mode with only two field components. The electric field component
Ez is in the
z-axis direction, while the magnetic field component is in the angular direction, and the phase difference between the electric field component and the magnetic field component is
. Where J
0(x) is the zero-order Bessel function, J
0′(x) is the derivative of zero-order Bessel function, and
,
is the first-order Bessel function. The j
01 is the first zero point of the zero-order Bessel function, and its value j
01=2.405. The Bessel function curves are shown in
Figure 5a. On the
=0 axis of the cavity, J
0(0) =1, it means that the electric field has the maximum value,
Ez (0,
z) =
E0. At the
=
R, the side wall of the cavity, because J
0(2.405) =0, the electric field is zero, i.e.,
Ez (
R,
z) = 0. The magnetic field at the
=0 axis, because
, it means that the magnetic field is zero, i.e.,
Hφ(0, z)=0. However, near the side wall of the cavity, where ρ=
R, J
1(2.405)= 0.5019, the magnetic field
Hφ(
R, z) has a bigger value, using the relation
, the
Hφ in Eq. (8) can be as
The amplitude of the angular magnetic field at
=
R is proportional to J
1(2.405) (
Figure 5a). The spatial distribution of the classical electric and magnetic fields in most spaces between the cavity axis and the cavity side wall is shown in
Figure 5b (note there is 90° phase difference between the electric field and the magnetic field). The field in the cavity is axisymmetric, there is no periodicity in both the
eφ-direction and the
ez-direction. The electron beam bunch is injected along the z-axis in a suitable half-period, which can be accelerated by the axial electric field
Ez. When the electric field peaks to accelerate the charged particles, the transverse circular magnetic field is nearly zero, since there is a 90° phase difference between the electric field
Ez and the magnetic field
Hφ.
4.2. Consideration to Construct the EM Field of the TM010 Mode with Photons
The intracavity field is a standing wave field. A single photon cannot be localized, a single LP photon pair cannot be localized either. Only co-volume identical LP photon pairs with opposite wave vectors k can be stationary since the wave vectors cancel out to zero, thereby the velocities also cancel out to zero (by the way, the photons in a MCR cavity are zero velocity photons). That is to say, the photon structure allowed in the resonant cavity can only be the standing wave 4-photon composite structure. Although, they have no translational velocity, but they do keep a spin velocity, i.e., a spin angular velocity.
Then we look at the resonant wavelength of TM010 mode, , and the photon diameter in free space, d=0.5032λ, now let < 2R. Compared with the cavity diameter 2R and cavity length L<2R, the photon size is not small and comparable to the cavity size, so the cavity volume can only accommodate one photon volume.
Furthermore, the photons in the cavity must be deformed into a cylinder to satisfy the Helmholtz equation and boundary conditions of the MCR cavity. The cylindrical photons of length L and radius R have the cavity axis as their symmetry axis. The electric-field substance vector, the magnetic-field substance vector, the wave vector and the spin angular momentum vector of the photon in free space are all Cartesian vectors [
17]. After entering the constraint cavity space, due to the interaction with the cavity wall, these vectors of each cylindrical photon turn into the orthogonal curve vectors (
Eez,
Heφ,
keρ) of the cylindrical coordinate system (ρ, φ, z),
eρ,
eφ,
ez are unit vectors on the ρ-, φ-, z-axis, respectively.
On the ρ=0 axis, J0(0) =1, J1(0)=0, so Ez(0,z)=E0cosωt, and Hφ(0,z)=0. Without magnetic field, it is a pure alternating electric field; And at the side wall of the cavity where r=R, J0(2.405) =0, J1(2.405) ≈0.519, so Ez (R, φ, z) = 0, Hφ (R, φ, z) = -ωε0(R/2.405)J1(2.405)E0sinωt. Without electric field, it is a pure alternating magnetic field. The electric-field and magnetic-filed components are mutually phase-shifted by 90° and superimposed orthogonally elsewhere.
For the amplitude of the electric field
Ez given by Eq. (8), the amplitude of the magnetic field
Hφ given by Eq. (9), it is observed in
Figure 5(a) that at x≈1.44, the zero-order Bessel function J
0(x) and the first-order Bessel function J
1(x) have a point of intersection, i.e., J
0(1.44) ≈J
1(1.44). Using this value, for any microwave frequency it can be calculated the amplitude ratio
Ez/
Hφ= 1/(ωε
0R/2.405) ≈377Ω, which is consistent with the wave impedance of the photon [
17].
Considering that the field in the cavity is axisymmetric, there is no periodicity in both the angular eφ direction and the longitudinal ez-direction. For cylindrical photons, the electric and magnetic field matter vectors are located in the cylindrical surface (z, φ); the wave vector and angular momentum along to the radial eρor -eρ.
In order to satisfy the conditions of pure electric field Ez (near axis) and pure magnetic field (near side wall), and to satisfy the conditions of phase difference of 90° between them, need two kinds of SW4-photon composite. The SWE4-P composite can provide a pure electric field along z-direction. The field substance distribution of its each photon along eρ- direction obeys function, is uniform along both the eφ- and ez-directions. The SWM4-P composite can provide a pure magnetic field Hφ along the eφ-direction. The field substance distribution of its each photon along eρ- direction obeys function, is uniform along both the eφ- and ez-directions.
The superposition of two kinds of SW4-P composite provides both the harmonic oscillation electric field along to the z-direction and the harmonic oscillation magnetic field along to the eφ-direction in the MCR cavity. The SWE4-P composite and the SWM4-P composite are configured in a 1:1 ratio, satisfying the principle of equal partition of EM energy in the cavity.
About the changes over time, demand that the SWE4-P composite obey cos
ωt function and the SWM4-P composite obey the sin
ωt function. Looking at the structure of the EM field given by Eq. (8) and (9) and comparing it with the electric and magnetic field expressions for the SW8-P composite structure given in
Section 3, one easily realizes that this TM
010 mode’s photon structure is a typical SW8-P composite structure. There is an inherent correlation between the SWE4-P composite and the SWM4-P composite, that is, the spatial orthogonal, the time phase difference of 90° relation, and the volume integral of its electric field energy is equal to that of the magnetic field energy (i.e., each half of the EM energy).
This SW8-P composite structure is the basic unit of the TM010 mode photon structure. Below we will discuss each of these in detail.
4.2.1. The SWE4-P Composite of the TM010 Mode
The EM field matter distribution of each photon in the cylindrical-shaped SWE4-P composite follows the zero-order Bessel
function along the radial ρ and is uniformly distributed along both the angular φ and the axis z. For a cylindrical photon, the electric and magnetic field matter vectors (
E,
H) of each photon are located in the cylindrical surface (φ, z), while the wave vector
k and angular momentum
j are in the radial (
e
ρ) direction. Right/left-spin photons in free space obey the
spin rule, how to implement the spin rule for right/left-spin cylindrical photons? We divide each cylindrical photon into an infinite number of differential volumes (d
V) by using the three orthogonal curve-surfaces ((r, φ), (φ, z), (z, r)). In each d
V the EM field matter vectors (
E,
H) of each photon spin-rotate about the local wave vector
k at ω according to the
spin rules like as in the Cartesian coordinate system as shown in
Figure 6.
Intracavity four cylindrical photons
E1H1,
E2H2,
E3H3 and
E4H4, at ωt=0°, are shown in
Figure 6 (a), (b), (c) and (d), respectively. The electric field substance vectors are all along the
z-axis, which becomes the manifest component; while the magnetic field substance vectors cancel out to zero, which become a hidden component. The direction of the electric field is along the
z axis, and the magnetic field direction is along the angular φ and connected the head and the tail. In order to see this clearly, take the same d
V as shown in (a’), (b’), (c’) and (d’) of
Figure 6. The
H1 of photon
E1H1 is along the -
eφ direction,
E1H1 right-spin, both its wave vector
k and its angular momentum
j are along the e
ρ direction; The
H2 of photon
E2H2 is also along the -
eφ direction,
E2H2 left-spin, its wave vector
k is along the e
ρ direction, but its angular momentum
j is along the -e
ρ direction; The
H3 of photon
E3H3 is along the
eφ direction,
E3H3 left-spin, its wave vector
k along the -e
ρ direction, but its angular momentum
j along the e
ρ direction; The
H4 of photon
E4H4 is along the
eφ direction,
E4H4 right-spin, both its wave vector
k and angular momentum
j are along the -e
ρ direction. In a word, the field substances superposition of the same d
V belonging to these four photons results in zero magnetic-field vector synthesis, zero total wave vector synthesis, zero total angular momentum synthesis and four times electric-field vector synthesis of single photon. This result is correct for the entire SWE4-P composite.
Figure 6 shows only the vector direction at the initial phase (ωt=0°) of photon
E1H1,
E2H2,
E3H3 and
E4H4 within the SWE4-P composite.
Figure 7(a), (b), (c) and (d) show the direction of the electric field substance vector and the magnetic field substance vector in the same differential volume belonging to four different photons at 0°, 90°, 180° and 270° phase points, respectively. Note that
H1 and
H3 are always in opposite directions and cancel each other out to zero, and
H2 and
H4 are always in opposite and cancel each other out to zero. The d
V, (a’), (b’), (c’), (d’) of each photon in
Figure 6 only corresponds to
Figure 7(a).
The result of superposition of four photons is that the total magnetic field is always 0, invisible, and the total electric field
E is a manifest component which is four times the intensity of the single photon. There is no net wave vector and no net angular momentum in any d
V, but the substances in each d
V which belongs to each photon keep independent spin. The
z-direction electric field of TM
010 mode is contributed by the SWE4-P composite alone. Obviously, it is the basic unit of the
z-direction electric field of TM
010 mode in the cavity. As a result, the pure electric field oscillates along the
z-direction with angular frequency ω. The electric field generated by the SWE4-P composite can be expressed as bellow:
4.2.2. The SWM4-P Composite of the TM010 Mode
Each photon in the SWM4-P composite is also deformed into a cylinder of length L and radius R. The EM field matter distribution of each photon in the SWM4-P composite follows the first-order Bessel
function along the radial ρ and is uniformly distributed along the angular φ and the axis z. The electric field
E and magnetic field
H of each photon are located in the cylindrical surface (φ, z), the wave vector
k and angular momentum
j are along the
eρ direction, as shown in
Figure 8. A significant difference from the SWE4-P composite is that the superposition of four photons results in that the total electric field component is zero. And the total magnetic field component along the
eφ direction, and oscillates harmonically at the angular frequency ω.
Take a d
V to illustrate the physical mechanism. As shown in
Figure 8, at ωt = 90° phase, the magnetic field
Hi (
i=1,2,3,4) belonging to the four photons of the SWM4-P composite are all along the -
eφ direction, while their electric field components are pairwise opposite to each other and cancel out to zero. Specifically, in the d
V, the magnetic field
H1 belonging to photon 1 is along the -
eφ direction, the photon
H1E1 left-spin, its wave vector
k1 is along the -
eρ direction, and its angular momentum
j1 is along the
eρ direction as shown in
Figure 8(a’); the magnetic field
H2 belonging to photon 2 is also along the -
eφ direction, the photon
H2E2 right-spin, both its wave vector
k2 and angular momentum
j2 are along the -
eρ direction as shown in
Figure 8(b’); the magnetic field
H3 belonging to photon 3 is along the -
eφ direction, the photon
H3E3 right-spin, both its wave vector
k3 and angular momentum
j3 are along the
eρ direction as shown in
Figure 8(c’); the magnetic field
H4 belonging to photon 4 is along the -
eφ direction, the photon
H4E4 left-spin, its wave vector
k4 is along the
eρ direction, its angular momentum
j4 is along the -
eρ direction as shown in
Figure 8(d’). In a word, in the same d
V belonging to the four photons, the superposition result is that the total electric field vector synthesis is zero, the total wave vector synthesis is zero, the total angular momentum synthesis is zero, and the total magnetic field vector synthesis is four times that of the single photon. This result is correct for the whole SWM4-P composite.
Figure 9 (a), (b), (c) and (d) show the direction of the electric field substance vector and the magnetic field substance vector in the d
V shared by four cylindrical photons at the four phase points of 0°,90°,180° and 270°, respectively. Note the
E1 and
E3 always cancel each other out to zero, the
E2 and
E4 always also cancel each other out to zero. The field synthesized by the four cylinder-photons is a pure magnetic field. The magnetic field produced by the SWM4-P composite harmonically oscillates at angular frequency ω along the
eφ direction,
The SWM4-P composite is the basic unit of the angular magnetic field of TM010 mode in the MCR cavity.
4.3. The SW8-P Composite Structure of the TM010 Mode
A superposition of a SWE4-P composite and a SWM4-P composite with a total of 8 photons as a basic unit constitutes the EM field of the TM
010 mode. The pure electric field
Ez near the axis is contributed by the SWE4-P composite alone, the pure magnetic field
Hφ near the side wall is by the SWM4-P composite alone, and the mixed electric and magnetic fields with a phase difference of 90° in other regions are jointly contributed by both SWE4-P composite and SWM4-P composite. The co-volume superposition of the SWE4-P and SWM4-P composites (total of 8 photons) as the basic unit provides the energy storage for the TM
010 of the MCR cavity. That is to say, the energy storage in the cavity increases step by step with the unit (
) of 8 photons. This is a result deduced from single photon structure model [
17].
The physical process that occurs in the cavity can be understood from the classical EM theory. As the electric and magnetic fields of eigenmode that satisfy the Helmholtz equation and boundary conditions of the MCR cavity, oscillating at angular frequency ω. The electric energy is converted into the magnetic energy, and the magnetic energy is converted into the electric energy, and so on, the electric and magnetic energies are converted into each other.
From the photon′s point of view, the physical process occurring in the cavity is the result of the EM field vector matter spin-rotate independently about their respective wave vectors () at the angular velocity ω in each dV of the eight cylindrical photons. This physical mechanism is more intuitive, concise and clear than the abstract image of “electric and magnetic energy can be converted into each other”. Of course, the classical theory of the EM field is still very accurate in its mathematical description, which is unrivaled by the photon′s point of view.