Hardware ProductsDetectorScientific‑grade CCD cameraEUV / Soft X-ray In-Vacuum CCD Camera - LOTTE-i Imaging Series

EUV / Soft X-ray In-Vacuum CCD Camera - LOTTE-i Imaging Series

Developed in Berlin, LOTTE is the latest innovation from German company greateyes, designed as an in-vacuum camera for spectroscopy and imaging in the extreme ultraviolet, vacuum ultraviolet, and X-ray energy ranges. LOTTE integrates state-of-the-art low-noise electronics and ultra-low-temperature cooling technology while maintaining a compact and lightweight design.

Germany

Model: LOTTE-i系列
Brand: greateyes

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Introduction

Originating from Berlin, LOTTE is the latest development by the German company greateyes, an in-vacuum camera for spectroscopy and imaging in the extreme ultraviolet (EUV), vacuum ultraviolet, and X-ray ranges. LOTTE integrates state-of-the-art low-noise electronics and ultra-low-temperature cooling technology while maintaining a compact and lightweight design. The new design allows flexible selection of readout speeds from 50 kHz to 5 MHz. The 18-bit analog-to-digital conversion utilizes the full dynamic range of the CCD sensor to achieve better performance and a higher signal-to-noise ratio. To match the requirements of different applications, the camera offers a variety of sensor types for user selection. Additionally, LOTTE's low noise makes it the ideal camera for extremely weak signal conditions, bringing unprecedented possibilities to your spectroscopy and imaging research.

Features & Advantages

1Hermetic design and ultra-high vacuum compatibility with quantum efficiency up to 98%
2Deep cooling to -100 °C
318-bit dynamic range
4kHz-MHz flexible readout rates with compact design

Specifications

Quantum efficiency

General Parameters

Readout Rate
50 kHz, 250 kHz, 1 MHz, 3 MHz (5 MHz for viewing mode; up to 20 MHz with multiple readout heads)
AD conversion resolution
18-bit
Linearity
Better than 99%
CCD epitaxial layer thickness
Standard 15 μm, deep depletion type 40 μm
Vacuum feedthrough flange
CF DN100 flange with D-sub connector and 6 mm water cooling inlet/outlet
Vacuum compatibility
Knife-edge sealing flange: 10-9 mbar (ultra-high vacuum)
Baking temperature
Max. +80 °C
Flange distance
1k1k series: 6 mm; 2k2k, 2k2k plus and 4k4k series: 5 mm (Note: all flange distances can be customized)
CCD sensor cooling
100 °C to 20 °C (water cooling only)
Temperature monitoring
On the CCD sensor and on the hot side of the thermoelectric cooler
Data transfer
Gigabit Ethernet GigE
Software
greateyes Vision software (Windows 7 / 10)
SDK and drivers
DLL for Windows; LabVIEW, EPICS, Linux, Python and Tango drivers (optional)
TTL interface signals
1 Exposure out, 1 trigger in
Power Supply
1k1k & 2k2k: 80-264 VAC (typ. 115/230), 47-63 Hz (typ. 50/60), max. 1.1 A (230 V) / 1.9 A (115 V) 2k2k plus & 4k4k: 85-264 VAC (typ. 115/230), 47-63 Hz (typ. 50/60), max. 1.9 A (230 V) / 3.8 A (115 V)
Certification
CE
Dimensions
9.0 cm (3.54ʺ) × 9.0 cm (3.54ʺ) × 23.5 cm (9.25ʺ) (W × H × L, 1k1k, 2k2k & 2k2k plus) 10.0 cm (3.94ʺ) × 11.0 cm (4.33ʺ) × 28.0 cm (11.0ʺ) (W × H × L, 4k4k)
Weight
4.5kg

Literature

1 references found

01
R. Loetzschnature24 January 2024

Quantum electrodynamics (QED), the quantum field theory that describes the interaction between light and matter, is commonly regarded as the best-tested quantum theory in modern physics. However, this claim is mostly based on extremely precise studies performed in the domain of relatively low field strengths and light atoms and ions1,2,3,4,5,6. In the realm of very strong electromagnetic fields such as in the heaviest highly charged ions (with nuclear charge Z ≫ 1), QED calculations enter a qualitatively different, non-perturbative regime. Yet, the corresponding experimental studies are very challenging, and theoretical predictions are only partially tested. Here we present an experiment sensitive to higher-order QED effects and electron–electron interactions in the high-Z regime. This is achieved by using a multi-reference method based on Doppler-tuned X-ray emission from stored relativistic uranium ions with different charge states. The energy of the 1s1/22p3/2 J = 2 → 1s1/22s1/2 J = 1 intrashell transition in the heaviest two-electron ion (U90+) is obtained with an accuracy of 37 ppm. Furthermore, a comparison of uranium ions with different numbers of bound electrons enables us to disentangle and to test separately the one-electron higher-order QED effects and the bound electron–electron interaction terms without the uncertainty related to the nuclear radius. Moreover, our experimental result can discriminate between several state-of-the-art theoretical approaches and provides an important benchmark for calculations in the strong-field domain.

Selection Guide

Select camera model

Select flange type

Camera standard accessories

Optional accessories and software

Typical Applications

  • Extreme ultraviolet (EUV) lithography

  • X-ray tomography / fluorescence imaging

  • Fourier transform holography

  • X-ray diffraction

  • X-ray phase-contrast imaging

  • Grazing-incidence small-angle X-ray scattering (GISAXS)


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