Let us introduce a rectangular coordinate system, the axis of which is aligned with the optical axis of the mirror, the plane coincides with its mean plane (horizontal plane), and the plane coincides with the plane perpendicular to the mean plane (vertical plane).

According to [2], the time-of-flight of an ion of charge and mass, moving along the optical axis of the mirror from the initial plane to an arbitrary plane, taking into account values up to the third order of smallness can be written as

Here

is the time-of-flight of the central particle,

is the total TOFCA of the mirror, is the initial energy spread of ions, is the axial distribution of the electrostatic potential, is the speed of the central particle, and

is the TOFCA coefficient of order, where the quantities and, determining the position of the effective plane of the mirror reflection and its reference planes of TOF focusing of order, respectively, are functions only of. Let us consider the particle moving along the axis with as the central particle. Here and below the subscript “0” denotes the values in the initial plane.

As it can be seen from (4), the condition of TOF focusing of ions by energy of order is written as

which means that TOF focusing is achieved when the plane (the ground plane) and (the TOF image plane) are located symmetrically with respect to the plane.

The plane is called the main plane of TOF focusing of the mirror [3]. Taking (5) into account, let us rewrite (2) as

where

is the time interval between the moments of intersection of plane by ions before and after reflection by the mirror. This time period is called the time interval of mirror focusing. The dependence of the time period of mirror focusing on its mass determines the value of its TOF mass dispersion

where

is the effective drift distance of the mirror.

If the condition

is fulfilled simultaneously with (5), all TOFCA coefficients are equal to zero, i.e. the TOF focusing in energy up to third order is realized.

According to [2], locations of mutually conjugate planes (the ground plane) and (image plane) are determined by the equation

Here is the radius of the mirror curvature, and are coordinates of the center of the mirror curvature and its vertex, and the subscript denotes the values in two mutually perpendicular planes, respectively.

When the centers of mirror curvature in two mutually perpendicular planes coincide or the center of curvature in the mean plane of the mirror coincides with its vertex in the plane perpendicular to the mean plane, i.e. if

or, (12)

stigmatic spatial focusing (SSF) is realized in the transaxial mirror.

Solving the system of equations (5) and (11) we find the spatial-TOF condition for the mirror:

The condition (13) determines the position of mutually conjugate planes and, for which spatial and TOF focusing are fulfilled simultaneously. For the electrostatic mirror with the given field distribution on its axis, there is only one pair of mutually conjugate planes that satisfy this condition [3].

As it is seen from (13), if the condition

or (14)

is fulfilled, spatial and TOF images of the object are formed in the same plane, i.e. spatial-TOF is fulfilled.

If conditions (5), (10) and (12) - (14) are fulfilled simultaneously, in the transaxial mirror the stigmatic spatial-TOF focusing (SSTOF) is realized.

In this section we used numerical calculations to determine the SSTOF conditions up to the second order in the three-electrode transaxial mirror (Figure 1). Each electrode of the mirror is a pair of parallel plates positioned symmetrically with respect to the median plane of the mirror.

Slits between the electrodes are cut along the arcs of concentric circles with the common centers of curvature, radii, where is the coordinate of the middle of the - th gap. Two modes of realization of SSF (12) conditions simultaneously with the TOF focusing of ions in energy up to the second order in such a mirror are considered. In the first mode SSTOF is achieved by superposition of the center of curvature in two mutually perpendicular planes, i.e. provided.

In the second mode SSTOF is obtained by superposition of the center of curvature of the mirror in the mean plane and its vertex in the perpendicular plane, i.e. provided. The trajectories (T) in the vertical plane for these modes are shown in Figures 2 and 3. As it can be seen from these figures, when the trajectories pass through the center of curvature of the mirror their direct and inverse branches are the same, and when trajectories pass through its vertex their direct and inverse branches are symmetrical with respect to the optical axis of the mirror [3].

The relations between geometrical and electrical parameters of the mirror defining the SSTOF conditions in the first and second modes are shown in Tables 1 and 2, respectively. Here are the potentials of the first, second and third electrodes, is the width of the second (middle) electrode, is the distance between the electrode plates, is the radius of the first circle. The values of geometric parameters are given

in units of, the electrical values—in units of potential. The origin of coordinates is located in the middle of the gap between the second and third electrodes.

As it seen from the above data, the effective drift distance of the mirror, hence, its TOF mass dispersion (8) in the second mode is two-three times higher than in the first mode. Moreover, the second mode has a higher capacity.

In this section, the four-electrode transaxial mirror, the second and the third (middle) electrode of which have the same width, are considered. Due to higher variety of the field distribution, in such a mirror it is possible to get SSTOF of higher quality.

Using numerical calculations we obtained the relationships between geometric and electrical parameters of the mirror that determine the conditions of TOF focusing up to the third order simultaneously with SSF, i.e. conditions.

The results of calculations are presented in table 3, where are the potentials of the first, second, third and fourth electrodes, is the width of the second and third (middle) electrodes, , , and have the same meaning as in the previous modes. The origin of coordinates is located in the middle of the gap between the third and fourth electrodes.

Let us consider the ion source consisting of the ionization region and the accelerating gap. Moving in the ion source, any ion with the initial energy will increase its own energy up to [4]:

Here is the electric field strength in the ionization region of width, produced by the pushing-out pulse, is the field strength in the accelerating gap of width produced by the accelerating potential difference, is the path traveled by the ion in the field of the pushing-out pulse. At the outlet of the ion source, ions have different energies due to the two factors: 1) different initial ion energies caused by thermal scattering, 2) different paths . Therefore, we can rewrite (15) in the form

where is the energy spread of ions in the package formed by the ion source.

Taking into account (16) the time-of-flight of an ion in the ion source can be written as

By simple transformations (17) can be represented in the form

where.

Expanding by powers of the small value (relative energy spread), and limiting by the order of smallness of not lower than the third order, we can write (18) in the form

where

is time-of-flight of the central ion, is the total TOFCA of the ion source determined by the equation

(21)

As it is seen from (21), under the condition

the term of the series proportional to, which makes the greatest contribution to the total TOFCA of the ion source, vanishes. The remaining part of aberrations of the ion source can be compensated by aberrations of the electrostatic mirror equal in magnitude and opposite in sign.

In the combined system consisting of the ion source and the electrostatic mirror, the total time-of-flight of the ion (in case the end of the accelerating interval of the ion source coincides with the initial plane of the mirror) taking into account (1) - (4) and (19) - (22) can be written as

where

Here

is the TOFCA coefficient of the combined system of order,

From (26) it follows that in the combined system the condition of the k-th order of TOF focusing of ions in energy is determined as

which means that TOF focusing is achieved when the plane, coinciding with the end of the second accelerating gap, and plane where the ions are recorded, are located symmetrically relative to the plane.

By analogy with the mirror let us call the plane the main plane of TOF focusing of the combined system. Taking into account (29) we can rewrite (24) in the form

where

is the time interval of focusing of the combined system.

TOF dispersion in mass and the effective drift distance of the combined system are determined by formulas similar to (8) - (9).

As an example calculations for TOF mass reflectron have been made, where the role of aberration corrector is played by the four-electrode transaxial mirror with two middle electrodes of the same width (Figure 4). The origin of coordinates is located in the middle of the gap between the third and fourth electrodes. The results of calculations are presented in Table4

Potentials on the second, third and fourth electrodes of the mirror, the width of its middle electrode, coordinates of the center of curvature of the mirror and the effective drift distance were calculated for different values of width of the accelerating gap of the ion source for the condition

When this condition is fulfilled in the plane coinciding with the plane, in the combined system TOF focusing up to the third order and stigmatic spatial focusing are achieved simultaneously.

In this case, the resolution of mass reflectron

will be limited only by the aberrations of the fourth and higher orders

where is the width of the packet of ions in the detector plane, is the 4-th order TOFCA coefficient.

It should be noted that in the conventional scheme of mass reflectron the resolution is limited by the ion packet width in the primary time focus [5]:

where is the focus distance of the ion source.

It follows that, other things being equal, in this mass reflectron the width of the ion packet in the detector plane is significantly (by an order or more) smaller than the width of the ion packet in the primary focus of the conventional mass-reflectron. This effect is caused by the compression of the initial width of the ion package by the mirror.