Solid-state cryogen-free cooling
Almost a century of demagnetization cooling
Magnetic refrigeration is a well-established technique that was proposed and first implemented back in the 1930s. It can be used to generate sub-Kelvin temperatures by exploiting the magnetic field dependence of the entropy of a spin system. This is illustrated in the following graph, which shows the entropy as a function of temperature for an ideal spin ½ system.
At high temperatures, the spins are randomly oriented and their entropy is constant. In contrast, at low temperatures, the entropy of the spin system is a function of the magnetic field B and the temperature T. In this regime, reducing the magnetic field from point (B) to point (C) under adiabatic conditions – i.e., while keeping the entropy constant– will result in a decrease of the temperature. For this reason, magnetic cooling is also known as “adiabatic demagnetization refrigeration,” or ADR for short.
ADR – Adiabatic Demagnetization Refrigeration
How Magnetic Cooling Works
A typical ADR configuration consists of a pre-cooling unit, nowadays typically a closed-cycle cryocooler, a heat switch, a superconducting magnet surrounding a solid-state cooling medium, and a sample platform.
At the beginning of the ADR process, the heat switch connecting the ADR with the pre-cooling unit is closed and both the cooling medium and the attached sample stage are cooled to the cryocooler base temperature of about 4 K.
While the heat switch is still closed, the cooling medium is magnetized by driving a current into the superconducting coil. The heat of magnetization is released and dissipated in the main thermal bath provided by the cryocooler.
Therefore, after the maximum magnetic field has been reached, the cooling medium will return to its base temperature. The entropy of the system is now essentially determined by the magnetic contribution of the spin sub-system of the cooling medium.
Then the heat switch is opened to break the thermal connection between the pre-cooling unit and the cooling medium. By reducing the magnetic field adiabatically, the temperature of the cooling medium drops thereby cooling the attached sample stage.
Usually, the medium is not completely demagnetized. Instead, the magnetic field is tuned to settle a target temperature and the remaining magnetic field is used to compensate for heat leaks from radiation, the support structure and wiring, as well as heat generated by the experimental setup. Thus, by further reducing the magnetic field the sample temperature can be stabilized with high precision for a limited period of time, the “hold time,” which is typically several hours.
Once the magnetic field has been reduced to zero, the ADR process can be repeated. The time to regenerate, i.e., to re-magnetize and relax the cooling medium will usually be 1-2 hours, resulting in typical duty cycles of 70 to 95%.
Cryogen-free, Accurate and Automatic
Take a look at our magnetic refrigerators
By combining closed-cycle cryocoolers and ADR, cooling into the mK regime can be implemented in a cryogen-free way. This is essential as the poor availability of helium-4 and notably helium-3 have recently caused a strong increase in the costs of operation and acquisition of low-temperature cryogenic equipment.
Additionally, compared to traditional cryogenic equipment, the absence of cryogenic liquids makes the operation of our tools safer, decreases maintenance costs and down times, and largely facilitates using cryogenic temperatures in both day-to-day laboratory work and industrial applications.
cADR – continuous Adiabatic Demagnetization Refrigeration
How to provide long-lasting sub-Kelvin temperatures without cryogens
To provide continuous cooling without cryogens, we consider a system with two ADR units, where, similar to the conventional “one-shot” ADR configuration, the first unit is connected to the main thermal bath via a heat switch. This time however a second ADR unit is added. It is connected on one end to the first ADR unit using another heat switch, and, on the other end to the sample stage. As shown schematically in the following figure, the two interconnected ADR units will work together to extract heat from the sample stage and to pump it into the 4 K main thermal bath.
Besides this serial two-stage configuration, many different cADR layouts with multiple ADR units can be realized, including serial or parallel configurations, and even combinations thereof. The optimal configuration depends on the demands of the experimentalist and the specific experimental conditions, and our tech team is happy to support you in choosing the best solution for your purpose.
At the beginning both the first and the second ADR unit are fully magnetized and connected through their respective heat switches. Therefore, the cooling media and sample stage initially have the temperature provided by the cryocooler.
First, unit 2 is decoupled from unit 1 and demagnetized, thereby cooling the sample stage down to the target temperature.
Then, the unit 1 is disconnected from the bath and demagnetized, too. It stabilizes a temperature well below the setpoint temperature of unit 2. Now the heat switch between the two ADR units is closed and unit 2 can be regenerated while at the same time the temperature of the sample stage is kept constant.
After unit 1 is depleted, the connection between the two units is opened again by opening the corresponding heat switch, and unit 1 is regenerated at the temperature of the cryocooler.
This procedure can be repeated infinitely to provide continuous cooling at the sample stage.
Top-loading cryostat for simple and fast low-temperature analysis
100 mK - 300 K
< 3 hours
Versatile, rack-mountable cryogenic platform
100 mK - 300 K
150 x 300 mm
At kiutra we believe that innovation and user-friendly design should not stop at cryogenics. Therefore, we are devoted to the manufacturing of highly automated cryostat systems, which may be operated also without expert knowledge. Thanks to the absence of liquid cooling media in the cooling process, our cryostats are very robust and fully automatic. Moreover, all systems can be controlled using a modern, user-friendly graphical software based on an open-source Python framework that can easily be adapted to your preferred measurement equipment and setups.
Automatic Sample Changer
A particularly outstanding feature developed by our cryo-engineers is the Automatic Sample Changer. The Sample Changer is a top-loading load-lock mechanism supplied as part of our L-Type Rapid cryostat. It allows to install sample pucks and cool them down to base temperature in less than three hours.
The Automatic Sample Changer offers several benefits:
First, by using several Sample Pucks different users can prepare their experiments in parallel. This is helpful if the preparation is complex and would block the operation of conventional systems and cause significant downtimes.
Second, the sample loading process is extremely fast. It takes just seconds to plug a Sample Puck into the Transfer Cage and secure the latter inside the vacuum lock, and a couple of minutes to automatically load the Puck to the low temperature stage, where it is cooled to the base temperature in less than 3 hours. The fast-cooling Pucks are particularly useful for the high-throughput screening of material samples and to accelerate the development of cryogenic devices.
Finally, as the sample preparation and sample loading does not involve any manual work at the cryostat or fragile probe sticks, the employ of the Sample Changer and Sample Pucks is an ideal solution for less experienced users, shared facilities, and in industrial environments.
Our video demonstrates how to work with the pucks and sample changer.
Top-loading cryostat for simple and fast low-temperature analysis
100 mK - 300 K
< 3 hours
Our Research Projects
kiutra actively contributes to the R&D of cryogenics and quantum technology
Together with Delft Circuits, kiutra has received funding from the European Eurostars programme, to develop a scalable platform for Quantum Technologies.
We are part of the MUNIQC-SC consortium, an initiative to build a quantum computer demonstrator based on superconducting circuits. Through a specific research project, we aim to develop, deploy and validate rapid testing setups for easy characterization and examination of cryo-electronic components and superconducting quantum circuits.
kiutra is happy to be part of the MATQu consortium, which has been awarded funding from the ECSEL Joint Undertaking for building a European eco-system for qubit materials, their processing and characterization.
The MARQUAND project is a joint effort of the Walter-Schottky Institut of TUM and kiutra GmbH. The goal of the project is the development and the cryogen-free operation of highly efficient quantum detectors.
A heat switch is a tunable thermal link. Heat switches are widely used in cryogenics and are a key component for every magnetic refrigerator. In a magnetic refrigerator, a heat switch is used to decouple the ADR cooling medium from its pre-cooling stage during the demagnetization cooling. In contrast, the heat switch is closed to conduct the heat of magnetization, which is generated during the regeneration process, into the pre-cooling stage.
There are several types of heat switches, each with different advantages and disadvantages. The most common types of heat switches are mechanical switches, gas-activated heat switches, and superconducting heat switches. Another distinction is between active and passive heat switches. For the first type, the switching process can be controlled by the operator, whereas for the latter, the switching process always happens at a certain, pre-defined temperature.
When operating a “one-shot” ADR cryostat, the cooling medium can provide cooling only for a limited amount of time, the “hold time”, which is determined by the cooling capacity of the medium.
After the cooling medium is magnetized and the heat of magnetization has been dissipated in the pre-cooling stage, the heat switch is opened and the cooling medium is partially demagnetized. During the demagnetization of the cooling medium its temperate drops. Once the target temperature has been reached, the demagnetization of the cooling medium is continued at a smaller field ramp rate which is chosen such as to compensate for thermal leaks through the support structure, thermal radiation, or customer setups. The total time available at the target temperature is referred to as “hold-time”. It ends once the magnetic field has been reduced to zero, i.e., when cooling medium is fully demagnetized and the cooling process terminates.
The hold time will vary as a function of temperature. so typically, when the system is operated at the lowest temperature, the system may still be operated at higher temperatures by re-magnetizing the cooling medium.
One major benefit of magnetic temperature control is that temperatures can be stabilized with high precision, as no valves, capillaries, or heaters are involved.
“One-shot” operation refers to the limitation of conventional ADR cryostats to provide cooling only for a limited amount of time, the “hold-time”, after which the cooling medium has to be regenerated. The regeneration process takes, depending on the cooling medium, 1-2 hours. During the regeneration, the cooling medium is typically warmed up to slightly above the temperature of the pre-cooling stage. As the “hold-times” of “one-shot” ADR cryostats are in the order of several hours, duty cycles between 70 and 95% can be achieved.
The limitation of temporary magnetic cooling is overcome in the first commercial multi-stage, continuous ADR (cADR) cryostats by kiutra.
A common concern regarding magnetic refrigerators is the presence of magnetic stray fields at the sample position during the operation of the cryostat. At kiutra we pay special attention to these magnetic fields to enable measurements also of very sensitive materials and devices.
In all our cryostats, we use compensated superconducting magnets to reduce the stray fields at the sample position and to minimize the magnetic interference between neighbouring cooling units in multi-stage systems.
In our L-Type Rapid, we took special care of the stray field by maximizing the distance of the ADR magnets and the sample stage. Together with our compensated magnet coils this ensures stray fields of less than 50 µT at the sample position, which is similar to the earth’s magnetic field. As in any other cryostat, mu metal shielding can be used to further reduce these small residual fields. This makes the L-Type Rapid a suitable tool to probe sensitive materials and devices, such as superconductors or quantum electronics.
It is also noteworthy, that the stray fields given in our specifications always refer to the maximum magnetic field in the cooling unit. In one-shot ADR cryostats, however, measurements are usually performed with the magnet operating at 0-30% of its maximum field, resulting in accordingly reduced stray fields. Similarly, in cADR systems, most of the magnets are operating at 10-30% of their maximum charge, which again leads to a reduction of the effective residual fields at the sample position.