Cell for Spectroscopy Cube S=6

Vibration transducers DN-4-M1 are designed to measure vibration by converting mechanical vibrations into electrical signals proportional to the vibration acceleration of an oscillating object. Vibration converters DN-4-M1 are used in conjunction with vibration measuring devices in factory and laboratory conditions.

The VT-002 vibration transducers are designed to convert the instantaneous value of the vibration acceleration of an object into an ICP signal of the IEEP standard.

Technical specifications Material: S-TIH53 (Ohara) Length, mm: 5 Height, mm: 1.5±0.02 Thickness, mm: 1.5±0.01 Refractive index, mm: 1.823 Effective focal length, mm: 0.91 Rear focal length, mm: 0.09 Transmission, %: >99.5 Power within the angle ± 0.7 mrad, %: >85 Antireflection coating, nm at one of the wavelengths from the range: 400-1500 Numerical aperture: 0.8 Surface quality λ = 633, nm: λ/4

Technical specifications Material: S-TIH53 (Ohara) Length, mm: 12 Height, mm: 1.0±0.01 Thickness, mm: 1.9±0.1 Refractive index, mm: 1.823 Optical aperture, mm2: 10.0*0.45 Back focal length, mm: 0.09 Transmission, %: >99.5 Pitch, mm: 0.5 Antireflection coating, nm at one of the wavelengths from the range: 400-1500 Numerical aperture: FA 0.5, SA:0.1 Surface quality at λ = 633 nm: λ/4 Residual deviation at full angle FW1/e2 mrad: <7, <10, <13

Vibration transducers DN-14 are designed to measure vibration by converting mechanical vibrations into electrical signals proportional to the vibration acceleration of an oscillating object. Vibration converters DN-14 are used in conjunction with vibration measuring devices in factory and laboratory conditions.

Vibration transducers DN-3-M1 are designed to measure vibration by converting mechanical vibrations into electrical signals proportional to the vibration acceleration of an oscillating object. Vibration converters DN-3-M1 are used in conjunction with vibration measuring devices in factory and laboratory conditions.

Technical specifications Material: S-TIH53 (Ohara) Length, mm: 13 Height, mm: 1 Thickness, mm: 1.5 Refractive index, mm: 1.823 Period, mm: 0.4 Radius at 45°, mm: 1.35 Transmission, %: ≥99.5 Antireflection coating, nm at one of the wavelengths from the range: 400-1500 Surface quality at λ = 633 nm: λ/4

Structurally, waveguide LPF 37-78 GHz are made on metal plates located in the center of the E-plane of the waveguide. These LFS can be used in conjunction with waveguide bandpass filters to increase the suppression of spurious signals and expand the upper band of the barrier. Basic properties Low bandwidth losses; A wide barrage strip. Operating conditions Operating temperature range from minus 10 up to 50 ° C; The relative humidity of the air is up to 98% at a temperature of 25 ° C. Technical specifications Waveguide cross section, mm 3.6×1.8 Bandwidth Fh-Fb at the level of -1 dB, GHz 60-78 The barrier band at the level of -30 dB, GHz 85-120 Bandwidth loss, 0.5-1.2 dB

Technical specifications Material: S-TIH53 (Ohara) Length, mm: 5.8±0.02 Height, mm: 1.5±0.02 Thickness, mm: 0.55±0.01 Refractive index, mm: 1.823 Pitch, mm: 0.5 Radius, mm: 1.49 Effective focal length, mm: 1.81 Back focal length, mm: 1.5 Transmission, %: >99.5 Antireflection coating, nm at one of the wavelengths from the range: 400-1500 Numerical aperture: 0.09 Surface quality at λ = 633 nm% λ/4 Residual deviation in the full angle FW1/e2 (for non-linear deviation of the laser diode), mrad: 90.0

The height of the optical axis of the furnace above the surface of the spectrometer table is 55 mm, the diameter of the samples is up to 21 mm, the length of the furnace in the direction of the optical axis is not more than 70 mm. The sample is installed in a screw-up cassette and is thermally insulated from the external environment by two screens on each side made of mylar and thin aluminum foil or graphlex. The total absorption of 14.4 keV radiation by the screens does not exceed 10-15%. The furnace is attached to the MS-1104Em spectrometer plate with non-falling screws and, if necessary (for example, when using a camera for recording conversion electrons or other equipment), it is easily removed and installed back. The folding mounting of the furnace allows for rapid replacement of samples without waiting for it to cool down, to perform operational calibration of the spectrometer without removing the furnace, and to measure the Mossbauer spectra of absorbers at room temperature outside it in geometry with a moving source or absorber, including in "compressed" geometry and using resonance detectors.