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Tramea lock-in modules

High-performance digital lock-in amplifiers

Single lock-in module
Single lock-in module with 1 frequency generator and 2 independent dual-phase demodulators

The lock-in modules let you modulate and demodulate any of the input and output signals available with frequencies up to 40 kHz. Up to 8 lock-in modules can be used independently from each other or synchronized in a phase coherent manner when the generation of multiple frequencies is required. With the multi-frequency option a single module can demodulate up to 8 harmonics of the same signal or independent input signals. The advantage of an internal lock-in detector over an external device is 

  • Higher resolution and dynamic range
  • Multifrequency and multi-input operation
  • Over 120 dB linearity
  • Over 100 dB dynamic reserve
  • No need for gain and attenuation switching
  • Steeper filters (up to 8. order) 
  • Up to 8 lock-ins, which can also be synchronized for phase-coherent operation
  • Lock-in can be synchronized with OC4. Measure STM current at the exact oscillation frequency of the probe
  • Synchronization with data acquisition when using Sync filtering
  • Integration avoids errors due to insufficient settling time with slow filter responses 
  • no additional noise source through external cabling
  • no potential grounding problems
  • Tandem-demodulation is straightforward to configure
  • flexible and simple setup
  • Guided filter set-up utility
  • Ability to turn on and off the excitation through software during the experiment
  • Ability to turn on and off the excitation for different bias ranges through software during the experiment

Applications range from regular transport measurements to multi-terminal Hall measurements, multifrequency measurements, simultaneous data acquisition with different time constants, dI/dV, inelastic electron tunneling spectroscopy (IETS), measurements of open and closed loop transfer functions and every type of phase sensitive measurements.

The lock-in filter array is also available for signals unrelated to lock-in measurements. The filters in the array are freely assignable, meaning that it is possible to use a subset of the filters for lock-in measurements and the remaining filters for generic purposes.

All lock-in modules also feature a sync output option. In addition to the main signal output, the lock-in module can generate a synchronization signal with the same frequency as the main signal. The amplitude can be configured independently from that of the main signal, and it is also possible to use harmonics of the main signal frequency as a sync signal. The sync signal is used to synchronize external instruments (for example other lock-ins, optical choppers,…) with the frequency of the internal lock-in. The output connector for the sync signal is user-selectable.

KEY FEATURES

  • Modulates any signal up to 40kHz
  • Demodulates any signal up to 100 kHz (R, phi and X, Y)
  • Up to 8 independent modules, synchronizable
  • Lock-in Modules can be synchronized to OC4 for acquiring signals at the oscillation frequency
  • Advanced signal filtering
  • Record transfer functions (bode plots)
  • Tandem-demodulation possible

Lock-in packages

TypeDesignationPart numberNumber of frequency generatorsNumber of dual-phase demodulators
Single lock-inLD5-121000022301

2

Dual lock-inLD5-2210000546724
Quad lock-inLD5-4210000585248
Octa lock-inLD5-8210000585388
Multi-demodulator option for LD5-1 and LD5-2LD5-MF2100005854Same as LD5-1 or LD5-28

Lock-in upgrade packages

TypeDesignationPart numberNumber of frequency generatorsNumber of dual-phase demodulators

Upgrade from LD5-1 to LD5-2

LD5UG1-221000058551 → 2

2 → 4

Upgrade from LD5-1 to LD5-4

LD5UG1-421000058561 → 42 → 8

Upgrade from LD5-1 to LD5-8

LD5UG1-821000058571 → 82 → 8

Upgrade from LD5-2 to LD5-4

LD5UG2-421000058582 → 44 → 8

Upgrade from LD5-2 to LD5-8

LD5UG2-821000058592 → 84 → 8

Upgrade from LD5-4 to LD5-8

LD5UG4-821000058604 → 88 → 8

Upgrade from LD5-1 with LD5-MF option to LD5-2MF

LD5UG1MF-2MF21000058611 → 28 → 8

Upgrade from LD5-1 with LD5-MF option to LD5-4 (includes LD5-MF option)

LD5UG1MF-421000058621 → 48 → 8

Upgrade from LD5-1 with LD5-MF option to LD5-8 (includes LD5-MF option)

LD5UG1MF-821000058631 → 88 → 8

Upgrade from LD5-2 with LD5-MF option to LD5-4 (includes LD5-MF option)

LD5UG2MF-421000058642 → 48 → 8
Upgrade from LD5-2 with LD5-MF option to LD5-4 (includes LD5-MF option)LD5UG2MF-821000058652 → 88 → 8

MADE FOR THESE METHODS

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SPECIFICATIONS

Tramea lock-in modules
Performance
Number of Frequency generators

1, 2, 4 or 8

Number of Demodulators

1, 2, 4 or 8 dual-phase demodulators assignable to any carrier

Modulation Frequency Range

100 mHz - 40 kHz

Demodulation Frequency Range

100 mHz - 100 kHz

Frequency Resolution

10 nHz

Phase Resolution

22 fRad

Demodulator Harmonic

1 - 32

Demodulator Filter Cut-Off Frequency

100 mHz - 20 kHz (corresponds to time constants between 18 s and 8 μs)

Demodulator Filter Slope

6, 12, 18, 24, 30, 36, 42, 48 dB/oct

Demodulator Output Resolution

32-bit

Demodulator Output Data Rate

1 MS/s

Sync Filter Frequency Range

100 mHz - 40 kHz

Linearity

120 dB

Dynamic Reserve

>100 dB

Operation
Reference

Any internal frequency generator or OC4

Demodulator Settings

Independent for each demodulator

RELATED PRODUCTS

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APPLICATION NOTES

Topological Insulator Josephson junctions
Topological Insulator Josephson junctions
In a topological insulator (TI), the electronic structure of the bulk reveals a unique topology that leads to the formation of conducting surface states with intriguing properties. The topological protection of the surface states and the possible emergence of Majorana fermions in superconductor/TI hybrid devices make these materials a leading candidate for use as a robust platform for future fault-tolerant quantum computation. The main challenge in creating these structures lies in the fabrication of an electrically transparent interface between the conventional superconductor and the topological insulator. A Josephson junction, formed by two closely spaced superconducting electrodes separated by a gap of less than 100 nm, can be used as a measure of the quality of the electrical interface. At low temperatures the superconducting electrodes induce superconductivity in the topological insulator by the proximity effect, with a finite Josephson current observed across a sufficiently narrow gap.
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Transport and RF-Reflectometry Measurements of CMOS Nanodevices
Transport and RF-Reflectometry Measurements of CMOS Nanodevices
Pioneering work on semiconductor quantum dots has shown that quantum dots are promising candidates as a building block (qubit) for quantum information and computation. Quantum dots are quasi-zero-dimensional nanostructures which can confine single electrons, whose spin or charge degree of freedom can then be used to represent quantum bits (qubits). Quantum computing approaches based on semiconductors can build upon mature micro/nano-fabrication technologies, which will be invaluable in scaling up to a large number of reproducible qubits with practical yields and integrated electronics. As part of the classical information technology industry, CMOS transistors have reached sufficiently small feature sizes that quantum effects can begin to play a dominant role. This motivates the exploration of quantum effects in such transistors fabricated using CMOS processes.
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PUBLICATIONS

  1. (2021) Quantum confinement of the Dirac surface states in topological-insulator nanowires
    Read more
  2. (2019) Gate Tunable Hole Charge Qubit Formed in a Ge/Si Nanowire Double Quantum Dot Coupled to Microwave Photons
    Read more

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