RHEED guns from STAIB Instruments provide unique electron optics systems for diffraction studies. Important options include differential pumping (DP) for use in high pressures and beam rocking to expand the sample positions that can be monitored. Short (S) or super short (SS) housings can be selected for confined spaces.
Energy range 500 eV to 20 keV
Beam current (max.) 80 µA
Beam size (min.) 60 µm at low current and 150 mm WD and max. energy
Working distance 50 mm – 750 mm
Differential pumping (DP) (optional)
In many growth environments, the vacuum conditions are not good enough to operate an electron gun.
RHEED systems from STAIB Instruments are available with a differential pumping option for pressures greater than 10-5 mbar. By utilizing a turbo pump (>40 l/s) attached to a special flange on the electron gun, the system continues to work well up to a few 10-3 mbar. Efficient pumping of the filament section of the source offers unbeatable versatility. For higher pressures, the double differential pumping option (TorrRHEED™) is available, which still allows the complete electronic control of the beam.
The differential pumping option is available on all RHEED systems from STAIB Instruments in the range of 15 eV to 60 keV.
For RHEED analysis, the electron beam must impinge onto the surface at grazing incidence.
The unique STAIB feature, beam rocking, allows precise adjustment and variation of the incidence angle using electronic controls, without moving the sample. Electron sources from STAIB Instruments are uniquely designed to allow this precise electronic control of the beam position using sophisticated electron beam deflection optics.
When equipped with the beam rocking option, specially designed optics shift the electron path off axis in the gun and refocus it onto the sample, maintaining the spot position. In this way, the incidence angle can be precisely controlled electronically without either modifications of the geometry of the gun or motion of the sample. The electron gun can be mounted on the vacuum chamber without using a bellows for mechanical adjustment. The beam rocking option is very helpful in critical cases where the sample position cannot be adjusted easily during the growth. In these cases, beam rocking allows precise variation of the incidence angle.
Additionally a full beam blanking option is available. Here the electron beam can be turned on and off using a TTL type input through a BNC connector.
The full beam blanking option can be used to keep the electron load on the sample very low. Electron bombardment of sensitive surfaces can be kept to a minimum. The blanking signal can also be triggered synchronously with external signals to improve the use of the electron source in the presence of stray magnetic fields by compensating their effect. The external trigger can also be utilized to synchronize with rotating samples, which is important for in situ monitoring in some deposition techniques.
STAIB Instruments has designed a patented system of beam steering that electronically controls the beam position and beam incidence angle.
With the patented STAIB TorrRHEED™, the incident angel can be changed with a unique double deflection system. The beam can easily be manipulated on the substrate without changing the mechanical alignment. This gives the operator the desired degrees of freedom for easy and simple alignment of the RHEED setup. RHEED diffraction conditions can be quickly and reproducibly fine tuned at any time, without the cumbersome mechanical manipulation approach used by other manufacturers.
The advanced beam steering is also used in the parallel beam shift option, which combines beam rocking (in X) and the parallel shifting of the beam (in Y). The RHEED beam can thus be used to analyze different positions on the substrate at the same RHEED angle (incidence and azimuth) (see RHEED for IBAD and RHEED for combinatorial deposition).
The computer control option for STAIB electron guns consists of two parts.
1: Power supply computer control plug
The electron source power supply is equipped with an optional computer connection plug for use with analog control signals. The electron source system can either be operated using the manual control dials, or by using the optional computer control. The control voltages can either be provided by 3rd party software through a suitable DAC interface, or by the STAIB computer control module.
2: STAIB computer control module
The STAIB computer control option includes the cables and microprocessor interface to connect to the power supply computer control plug. The STAIB software sends the input signals to the power supply to control the system functions. Full parameter sets can be stored, modified, and reused. The advanced version of the STAIB computer control module can retrieve and copy the adjusted values from the manual control dials, providing the user with previously unavailable ease of use.
The option runs under the WindowsTM XP, WindowsTM 7, WindowsTM 10 operating systems, using a USB connection.
RHEED computer control includes a microprocessor interface module and a software package, and makes use of the RHEED very precise and repeatable. User’s parameters can be saved and retrieved, the beam can be turned on and off using the beam blanking option, and the incidence angle can be adjusted using the optional beam rocking feature of the gun.
The Beam Current Controller (BCC) is a microcontroller based unit used to regulate the electron beam current of the electron gun, as used in RHEED or AUGER techniques.
Regulation of the electron beam current to a fixed, precise, user-adjusted value is important when the electron gun is working in a higher pressure range and when using reactive gases in the vacuum chamber. Once adjusted, the BCC will regulate the beam current to the assigned value, even after gun parameters like beam energy or focus are modified. Operating values can be saved and will be kept after restarting the BCC module, ensuring identical experimental conditions.
A RHEED system from STAIB Instruments can be equipped with magnetic shielding. The shielding may be necessary because a magnetic field influences the electron beam. A static or DC magnetic field will shift the beam and an alternating field will wobble the beam. This can cause fluctuations in beam position, size and current.
The magnetic shielding is made of a highly ferromagnetic material. For this reason, it can be used to shield low frequency magnetic fields from the surrounding environment.