Low Temperature Hall Effect Test System

Low Temperature Hall Effect Test System

DX-1000L Low Temperature Hall Effect Test System
1. Offers a variety of low-temperature range options (e.g., 78K-325K / 4K-525K).
2. Comes standard with integrated low-temperature equipment, providing magnetic fields of up to 1 Tesla, with optional electromagnets available for higher magnetic fields.
3. Precise temperature control with fast heating and cooling rates.
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Description
Product introduction

 

DX-1000L Low Temperature Hall Effect Test System consists of an electromagnet, electromagnet power supply, high-precision constant current source and high-precision voltmeter, Hall effect sample holder, standard sample, high and low temperature Dewar, temperature controller, and system software.

 

DX-1000L Low Temperature Hall Effect Test System is used to measure important parameters such as carrier concentration, mobility, resistivity, and Hall coefficient of semiconductor materials. These parameters must be controlled in advance to understand the electrical properties of semiconductor materials. Therefore, the Hall effect test system is an important tool for understanding and researching semiconductor devices. and electrical properties of semiconductor materials.

 

The experimental results are automatically calculated by the software, and parameters such as Bulk Carrier Concentration, Sheet Carrier Concentration, Mobility, Resistivity, Hall Coefficient, and Magnetoresistance can be obtained at the same time.

 

The DX-320 effector specially developed for this instrument system integrates a constant current source, a six and a half microvolt meter and a complex switching relay-switch for Hall measurement, which greatly reduces the connection and operation of the experiment. DX-320 can be used as a constant current source and microvoltmeter alone.

 

Technique Data of DX-1000L Hall Effect Test System

 

Physical parameters

Carrier concentration

5*1012 ~ 51*1020cm-3

mobility

0.1~108cm2/volt*sec

Resistivity range

5*10-5~5*102Ω.cm

Resistance range

10 m Ohms~ 6MOhms

Hall coefficient

±1*10-2~±1*106cm3/C

Magnetic field environment

Magnet type

Variable electromagnet

Magnetic field strength

The maximum magnetic field is 20000Gs when the distance between N and S is 10mm;
N, S maximum 13000 Gauss at 20mm spacing;
The maximum magnetic field is 10000 gauss when the distance between N and S is 30mm;
Uniform area: When the air gap is 60mm, the diameter is 10mm and the uniformity range is 1%.

minimum resolution

0.1GS

Magnetic field range

0-1T

Optional magnetic field environment

Customization is available

Electrical parameters

Sample current

0.05uA~50mA (adjust 0.1nA)

Measure voltage

0.1uV~30V

Temperature environment

Temperature adjustment

0.1K

Warm zone

78K-325K, 4K-325K (optional)

Testable materials

Semiconductor material

SiGe, SiC, InAs, InGaAs, InP, AlGaAs, HgCdTe and ferrite materials, etc.

low resistance material

Graphene, metals, transparent oxides, weakly magnetic semiconductor materials, TMR materials, etc.

High resistance material

Semi-insulating GaAs, GaN, CdTe, etc.

 

Parameters of each component

 

High precision electromagnet:

 

  • Pole diameter 100mm;
  • The maximum magnetic field is 20000Gs when the air gap is 10mm;
  • The maximum magnetic field is 13000 Gauss when the air gap is 20mm;
  • The maximum magnetic field is 10000 gauss when the air gap is 30mm;
  • Uniform area: when the spacing is 60mm, the diameter is 10mm, and the uniformity range is 1%;
  • Weight 110 kg, including bracket and wheels.

 

High-precision bipolar constant current power supply

 

  • Output: ±10A±80V;
  • Power: 800W;
  • The power supply output current can continuously change between positive and negative rated maximum current;
  • The current can smoothly cross the zero point without switching commutation;
  • Four-quadrant operation of output current and voltage (suitable for inductive loads);
  • The current change rate can be set in the range of 0.0007~0.3 F.S./s (F.S. is the rated maximum output current);
  • Current stability: better than ±25ppm/h (standard type); better than ±5ppm/h (high stability type);
  • Current accuracy: ± (0.01% set value + 1mA)
  • Current resolution: 20 bits, for example, 15A power supply, the current resolution is 0.03mA;
  • Source effect: ≤ 2.0×10-5 F.S. (when the power supply voltage changes by 10%, the output current changes);
  • Load effect: ≤ 2.0×10-5 F.S. (when the load changes by 10%, the output current changes);
  • Current ripple (RMS): less than 1mA.

 

High precision gauss meter:

 

  • Accuracy: ±0.30% of reading;
  • Resolution: 0.01mT Range: 0-3T;
  • Probe thickness: 1.0mm;
  • Length: 100mm digital;
  • Rs-232 interface data reading software with GP3 probe;
  • All-aluminum non-magnetic bracket 5-70mm adjustable.

 

Cryostat:

 

  • 80K-293K high and low temperature vacuum container;
  • DX301 thermostat temperature control (65k-600k);
  • Vacuum pump K25 vacuum pump.

 

Constant current source and test table

 

  • Constant current source range: ±50nA-±50mA;
  • Resolution 0.1nA, continuously adjustable within the range;
  • High-precision voltage data acquisition instrument range 0. 1uV-30V;
  • Accuracy: 0.01%;
  • Built-in test matrix conversion card;
  • Ohmic contact kits Make kits based on ohmic contacts of different materials.

 

Introduction of control software:

 

One-button measurement operating system, you only need to set a few sample parameters and the required temperature, and then you can measure automatically with one button, no need to keep an eye on it. When measuring, you only need to set the current passing through the sample, the magnetic field size of the magnetic field environment where the sample is located, and the thickness of the sample to measure. If you need to control the temperature, turn on the temperature setting to set the required temperature, and select the output power to control the temperature. Temperature control takes a short period of time (about 1 minute). After the temperature is stable, various parameters at this temperature can be measured. The data can be plotted and exported to EXCEL for post-processing and use.

 

Deliver, shipping and serving

 

We support shipping by sea, air, and express delivery. Our services cater to a range of shipping needs, ensuring that our customers can choose the best option for their specific requirements. We aim to meet their expectations by providing cost-effective and timely deliveries.

 

In addition to our shipping capabilities, we also prioritize quality customer service. Our team is always ready to provide timely and relevant information about your shipment, making sure to keep you informed every step of the way.

 

FAQ

 

Q: What is the lowest temperature that the low-temperature Hall Effect system can achieve?

A: The low-temperature Hall Effect system typically operates within a specific temperature range, but the lowest temperature achievable may vary depending on the system's design and specifications.

Q: How does the low-temperature Hall Effect system maintain stability and accuracy in cold environments?

A: The system's stability and accuracy in cold environments are typically ensured through rigorous calibration procedures, precise temperature control mechanisms, and the use of high-quality materials resistant to temperature fluctuations.

Q: Can the low-temperature Hall Effect system be used for superconducting material characterization?

A: Yes, many low-temperature Hall Effect systems are designed to accommodate superconducting materials and can provide valuable insights into their electronic properties at extremely low temperatures.

Q: Are there any special considerations for sample preparation in the low-temperature Hall Effect measurements?

A: Yes, sample preparation in low-temperature Hall Effect measurements may require additional precautions to ensure the integrity of the sample and accurate measurements. This may include handling the samples in a controlled environment to prevent contamination or degradation.

Q: How can I interpret the Hall Effect measurements obtained at low temperatures?

A: Interpreting Hall Effect measurements obtained at low temperatures requires understanding the unique electronic properties of materials at those temperatures. This interpretation often involves comparing the experimental results with theoretical models and considering factors such as carrier concentration, mobility, and conductivity.

 

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