Multi-target RF & DC sputtering System
High frequency antenna and waveguide design
Low-noise chip carrier design for the transport set-up
Micro bonding
Broadband Ferromagnetic Resonance Spectroscopy (self-made)
Spin-Torque Ferromagnetic Resonance Spectroscopy (self-made)
Vector Network Analyzer (VNA)
Room-temperature Transport measurement system
Cryo-free (9T-2K) Transport & FMR system (CFMS)
Optical (Microwriter DMO) and e-beam lithography
Pulsed Laser deposition (PLD)
Superconducting quantum interference device (SQUID)
Physical Property Measurement System (PPMS-Quantum Design)
XRD (including High Resolution & Reciprocal Space Mapping), SEM, EDAX, XPS, FE-SEM, VSM
LabVIEW to interface all type of instruments
Little experiences with atomic and magnetic force microscopies (AFM, MFM), transmission electron microscopy (TEM)
Micromagnetic Simulations (OOMMF, muMAX3)
High frequency (GHz) Simulation in Ansys & TxLine
Device Design in AutoCAD, Eagle
A little experience with python, MATLAB
Numerical analysis and programming (M.Sc.)
Electronics (M.Sc.)
Thermal and statistical physics (Engineering and M.Sc.)
Physics for Engineers (Engineering)
Technology Museum Lab (Engineering)
Physics Lab (Engineering)
Preparatory Course (Engineering)
Partially Supported-Mr. Manish Kumar Singh (M.Sc.)- Micromagnetic Simulation in a FM/HM bilayer-2020
Partially Supported-Mr. Ajit Kumar (M.Sc.)- 1/f Noise spectroscopy-2021
Mr. Adarsh Tripathi (M.Sc.)- Investigation of Active polymer like system in presence of electric field-2023
Mr. Apurba Mondal (M.Sc.)-Understanding the spin torque FMR in Magnetic Heterostructures-2024
Sputtering is a plasma-mediated deposition procedure wherein high-energy ions are propelled towards a designated target. Upon impact, these ions induce the ejection, or sputtering, of atoms from the target surface. Subsequently, the sputtered atoms traverse towards a substrate, where they integrate into the evolving film. This process serves as a method for the thin film deposition, leveraging the kinetic energy of accelerated ions to facilitate the dislodgement and subsequent deposition of target material onto a specified substrate.
Magnetic thin films play crucial roles in contemporary spintronics and magnonics research, as well as in emerging technologies like magnetic memory architectures, sensor arrays, logic circuits, and microwave signal processing platforms. Despite the prevalence of traditional quasi-static methodologies such as vibrating sample magnetometry for thin film characterization, investigating microwave-driven magnetization dynamics offers a complementary avenue for comprehensive analysis.
By scrutinizing the intricate interplay of microwave-induced magnetization dynamics within thin film configurations, researchers unlock a rich array of material parameters, including the gyromagnetic ratio (γ), damping (α), inhomogeneous broadening (ΔHo), and exchange stiffness (A). Proficiency in elucidating these parameters is essential for fine-tuning the functional characteristics of magnetic thin films across diverse application domains and advancing the frontiers of magnetic materials science.
The integration of static and dynamic characterization modalities transcends traditional analytical paradigms, offering a nuanced understanding of the intricate magnetic behaviors exhibited by thin films. This multidimensional approach not only facilitates tailored optimization of thin film properties to meet specific technological requirements but also catalyzes exploration into novel emergent phenomena within the magnetic materials landscape.
Furthermore, employing FMR spectroscopy with either stripline or coplanar waveguides enables measurements spanning a broad frequency spectrum extending over tens of gigahertz. These extensive bandwidth measurements provide significant advancements in precisely extracting the aforementioned material parameters. Specifically, broadband measurements are indispensable for scrutinizing the frequency-dependent behaviors of the resonance linewidth and discerning the intricate interplay between intrinsic and extrinsic mechanisms influencing magnetic damping.
Experimental details:
This paragraph provides a succinct overview of the underlying physics governing microwave magnetization dynamics, outlines the methodology for conducting and interpreting broadband Ferromagnetic Resonance (FMR) measurements.
The core component of a broadband FMR spectroscopy setup, depicted in Figure 2(b), is the coplanar waveguide (CPW). The CPW efficiently transmits microwave signals from a radio frequency (RF) source across a wide range of frequencies. CPWs can transmit frequencies from 8kHz-40 GHz. In close proximity to the CPW, a microwave RF magnetic field (HRF) is generated, which can resonantly excite a magnetic sample at an appropriate magnetic field (HDC) and frequency.
Given that RF magnetic fields are localized near the CPW, it's crucial to place magnetic films face down on the CPW to maximize coupling and resulting signal. Additionally, to prevent the sample from shorting-out the CPW, a thin insulating layer (such as sputtered SiO2 or spin-coated photoresist) is often applied to the sample. Alternatively, a single layer of transparent tape on the CPW can serve as an insulating barrier.
Optimal excitation occurs when the HRF is perpendicular to the magnetization of the sample, hence HRF should be perpendicular to HDC, as illustrated in Figure 1(a). Typically, measurements are conducted at a fixed frequency while sweeping HDC to eliminate any dominant frequency-dependent background response that might obscure the relatively weak FMR response of the sample. As HDC is swept through the resonance condition, the magnetization begins to resonantly precess, absorbing energy from the CPW. This decrease in transmitted RF energy during resonance field sweeping is converted to a DC voltage by a broadband RF diode, resulting in an absorption response.
To enhance the signal-to-noise ratio (SNR), a lock-in detection technique is commonly employed, necessitating signal modulation at a known frequency. This modulation is achieved by an additional set of Helmholtz coils powered by an AC source, producing a small (~3 Oe) modulation (HAC) to the much larger HDC. Thus, with this modified measurement scheme, we can effectively measures the derivative of the transmitted power (dP/dHDC), as illustrated in Figure 1(b).
The electronic components (AC Source, RF Source, RF Diode, and Lock-in) depicted in Figure 1(a) are conveniently integrated within the FMR set-up, as shown in Figure 2(a), along with the necessary electronics to control the HDC & Resonance frequency. The whole system is fully automated with compatible programming language.
Introduction:
The Mini Cryogen-Free Magnet System (CFMS) is a versatile, closed-cycle platform that enables precise control of magnetic field and temperature — without using liquid helium or nitrogen. It forms the backbone of modern condensed matter and spintronics research by providing a stable, cryogen-free environment for exploring fundamental physical phenomena.
At its heart is a superconducting magnet, cooled by a closed-loop helium refrigeration system, achieving magnetic fields up to ±9 Tesla and temperatures from 1.6 K to 400 K. This compact and maintenance-free system enables long-duration experiments under extreme conditions with high reproducibility.
Magnetic Field: ±9 T
Temperature Control: 1.6 K to 400 K
Cryogen-Free: Closed-loop helium cooling
Low Noise Environment: Suitable for sensitive electrical and magnetic measurements
CFMS provides the physical conditions required for various advanced measurements when integrated with external instruments (lock-in amplifiers, vector network analyzers, source-meters, etc.).
🧲 Magnetization & Spin Dynamics
FMR – Ferromagnetic Resonance
ST-FMR – Spin Torque Ferromagnetic Resonance
AC Susceptibility & Magnetic Moment
⚡ Hall Effect & Transport Measurements
Harmonic Hall Measurements (1st, 2nd, 3rd Harmonics)
AHE – Anomalous Hall Effect
PHE – Planar Hall Effect
OHE – Ordinary Hall Effect
QAHE – Quantum Anomalous Hall Effect
QHE – Quantum Hall Effect
🔄 Spintronic Phenomena
SHE – Spin Hall Effect
ISHE – Inverse Spin Hall Effect
Spin Seebeck Effect
Thermal Spin Transport
Nonlocal Spin Valve & Spin Diffusion Experiments
⚙️ Other Applications
Magnetoresistance (TMR, GMR, AMR)
Resistivity, IV Characteristics
Magneto-thermoelectric effects
Light-induced transport/photoresponse under field
“From fundamental quantum effects to applied spin transport — CFMS enables it all.”
Pulsed Laser Deposition (PLD) is a versatile and precise thin film deposition technique widely used in materials science to grow high-quality films of complex materials. It is especially favored when creating films that require maintaining the exact chemical composition of the target material.
How PLD Works
At the core of PLD is a high-powered pulsed laser—often an excimer or Nd:YAG laser—that delivers very short bursts (pulses) of intense light energy onto a solid target made of the material to be deposited.
When the laser pulse hits the target surface, the energy is absorbed, rapidly heating and vaporizing a tiny portion of the target.
This process creates a plasma plume, a highly energetic cloud of vaporized atoms, ions, electrons, and molecular fragments.
The plasma plume expands away from the target in a vacuum chamber or a controlled gas environment (like oxygen or argon), depending on the desired film properties.
A nearby substrate (a clean, flat surface) is positioned to collect the vaporized particles.
As these particles reach the cooler substrate, they condense and nucleate, gradually forming a thin film layer by layer.
Key Parameters Controlling PLD
Several factors influence the quality and characteristics of the deposited film:
Laser parameters: Wavelength, pulse duration (usually in nanoseconds), energy density (fluence), and repetition rate.
Target composition and structure: The chemical makeup and crystallinity of the target directly influence the film’s properties.
Substrate temperature: Heating the substrate can improve film crystallinity and adhesion.
Ambient gas and pressure: The background gas affects the plasma dynamics and chemical reactions during film growth, which is critical for oxide or nitride films.
Target-to-substrate distance: Determines how the plume expands and deposits material uniformly.
Advantages of PLD
Stoichiometric transfer: PLD often transfers the exact chemical composition of the target to the film, making it ideal for complex or multicomponent materials like oxides and superconductors.
Versatility: It can deposit a wide variety of materials including metals, semiconductors, insulators, and complex oxides.
High-quality films: PLD films can have excellent crystallinity, smooth surfaces, and well-defined interfaces.
Rapid switching: Changing targets is fast, allowing multi-layer structures and heterostructures to be grown by sequential ablation.
Applications of PLD
PLD is widely used in research and industry for fabricating:
Superconducting thin films: For quantum devices and sensors.
Magnetic thin films: For spintronics and memory devices.
Transparent conducting oxides: Used in solar cells and displays.
Dielectric and ferroelectric films: For capacitors and non-volatile memory.
Optical coatings: Anti-reflective and high-reflectivity layers.
Complex multilayers and heterostructures: For advanced electronic and spintronic devices.
Pulsed Laser Deposition is a powerful method that uses short, intense laser pulses to vaporize material from a target, forming a plasma plume that deposits precise, high-quality thin films onto substrates. Its flexibility and ability to preserve material composition make it invaluable for creating complex thin films in cutting-edge technology research.
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(c)
Picture 1 (a) Class 1000 Clean Room, (b) Abhishek and Athira going for Microwriter, (c) Abhishek operating thermal evaporator for deposition of Pt, (d) Patterned IDE ready for deposition
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(d)
Testing device
OHE/SHE/AHE/PHE/QHE/QAHE/ANE Testing device
Testing Devices for 1/f Noise and Gating
Second Harmonic Hall measurement
Hall Voltage measurement (Vxy)
Marks of wire Bonding (wedge)
For RF Application
Harmonic hall Measurement
A key part of my experimental workflow involves micro/nanofabrication using the Microwriter DMO, a high-precision maskless lithography system. This system allows direct writing of custom patterns onto substrates using a focused UV laser, eliminating the need for physical photomasks — which makes it ideal for prototyping and fine-tuning device structures.
At the core of lithography lies the principle of selective light exposure on a photoresist-coated substrate, followed by development to create patterns for subsequent processing like etching or metal deposition. With the DMO, I typically use a 0.6 µm lens, which gives me the resolution needed for extremely small features.
My Lithography Work:
Patterning sub-micron to 2 µm wide current channels for Hall bar devices.
Performing lithography directly on exfoliated 2D materials (like flakes of graphene or TMDs), aligned carefully under a microscope.
Implementing grayscale lithography to fabricate structures with variable depth and profile — an advanced technique especially useful on uneven flake surfaces.
Working on ultra-small substrates, as tiny as 1 mm × 1 mm and 2 mm × 2 mm, where handling and alignment become extremely challenging.
Despite the difficulty of working with such small-scale substrates and fragile 2D materials, I successfully developed a robust and repeatable recipe — a result of countless iterations, failed patterns, and deep troubleshooting.
Photoresist & Process Details:
I use AZ5214E, a versatile image reversal photoresist, compatible with the fine-resolution patterns I require.
The development process uses a compatible developer (like AZ 726 MIF) carefully timed to avoid over- or under-development.
Challenges & Breakthroughs:
Working on such a micro-scale often led to:
Incomplete development,
Pattern distortion due to substrate curvature,
Lift-off failure due to adhesion issues.
But over time, through extensive process optimization — including adjusting baking times, exposure doses, and development parameters — I overcame these hurdles. I now have a reliable process for high-resolution lithography on both conventional and exotic substrates.
I'd love to show a few images of failed vs. successful patterns — they tell a story of trial, error, and eventual success.
Lithography is a cornerstone process in micro/nanofabrication, and when it fails, it often does so in subtle but devastating ways. Working extensively with the Microwriter DMO, I've encountered and resolved many challenges while patterning sub-micron features, Hall bar structures, and 2D material-based devices.
Here are the key factors that can cause patterning failures or defects, based on hands-on troubleshooting:
1. Substrate Issues
Substrate Size & Handling
When working with very small substrates (e.g., 1 mm × 1 mm, 2 mm × 2 mm), even minor misalignments or motion during spin coating or exposure can lead to total pattern failure.
Surface Contamination
Dust, moisture, or even leftover exfoliation tape residue can prevent photoresist adhesion or cause uneven development.
2. Photoresist Coating Problems
Non-uniform Spin Coating
On small or non-standard substrates, achieving a uniform photoresist layer is difficult. This can lead to incomplete exposure or irregular pattern formation.
Incorrect Bake Parameters
Overbaking or underbaking (softbake/hardbake) can alter resist sensitivity or cause cracks, especially when using AZ5214E for image reversal processes.
3. Exposure Parameters
Wrong Focus Height or Dose
In the Microwriter DMO, incorrect z-height calibration, lens choice, or exposure dose can result in:
Overexposed (merged) features,
Underexposed (faint or incomplete) lines.
Feature Size vs Lens Resolution Mismatch
Using a larger lens for fine patterns can blur or distort small features (I typically use the 0.6 µm lens for sub-micron Hall bars and fine current channels).
4. Development Failures
Incorrect Developer Concentration or Time
Using AZ 726 MIF with AZ5214E, if development time is off by even 10–20 seconds, it can lead to:
Overdevelopment: lifting fine features or damaging edges.
Underdevelopment: pattern not fully cleared.
Aggressive Agitation or Rinsing
Especially on exfoliated flakes or grayscale patterns, excessive agitation during development can cause pattern delamination or loss.
5. Grayscale & Flake Patterning Specific Challenges
Non-Uniform Substrate Topography
Patterning on 2D flakes involves aligning on non-flat, sometimes transparent regions. This makes both focus and exposure intensity tricky to control.
Resist Thickness vs Depth Profile
For grayscale lithography, if the resist thickness or exposure gradient isn't tuned properly, the resulting 3D structures are unpredictable or fail to form.
6. Equipment or Environmental Issues
Stage Drift or Vibration
During long exposures or multi-layer alignment, any mechanical instability causes pattern shift or blur.
Optical Path Dust or Misalignment
A dirty lens or misaligned beam in the Microwriter DMO can cause uneven exposure across the pattern.
After working with dozens of 2D flakes and nanoscale devices, I've developed a reliable process recipe — but it came after many rounds of optimization. I've also documented and analyzed failed patterns to identify causes, including:
Lift-off artifacts,
Residual resist in narrow gaps,
Feature collapse during drying.
Sharing those failure cases and learning from them has been essential to building robust, reproducible fabrication processes.
3mm*3mm Wafer Un-even coated PR
2mm*2mm Wafer Un-even coated PR
1mm*1mm wafer almost developed
Un-even coated PR
Over developed
Over developed
Dust particles on Voltage leads
Perfect Device
Wire bonding is a critical technique in micro/nanoelectronics — and especially so in spintronic devices, where device dimensions are small and signal fidelity is highly sensitive to contact quality. In my research, wire bonding plays an essential role in establishing reliable connections between fabricated devices and external measurement systems, such as probe stations and cryogenic setups.
What is Wire Bonding?
Wire bonding is a method of creating electrical interconnects between a microchip or substrate and a larger circuit, using thin metal wires. This is typically achieved using a combination of pressure, heat, and ultrasonic energy, depending on the bonding method.
The choice of bonding technique and wire type depends on device geometry, material stack, operating conditions (such as cryogenic temperatures), and signal requirements.
Bonding Techniques & Tools I’ve Worked With:
I have hands-on experience working with:
West-Bond (manual)
TPT Wire Bonder
F&S Bondtec (manual and semi-automated systems)
And I've used the following wire bonding methods:
Wedge Bonding: Common for fine-pitch layouts and aluminum wires.
Ball Bonding: Ideal for gold wires; quicker and more automated.
Ribbon Bonding: Used in high-frequency applications due to its broader contact area.
Wire Types I’ve Used:
Aluminum wire – typically for wedge bonding, suitable for low-temperature and spintronic setups.
Gold wire – used in ball bonding for high-quality, low-resistance connections.
Gold ribbon – occasionally used for RF/microwave applications.
Ensuring Bond Quality in Spintronic Devices
Since I work with micro and nanoscale spintronic devices, bond quality is not just important — it's critical. A weak or unstable bond can drastically affect:
Contact resistance, leading to errors in resistance and Hall measurements.
Signal-to-noise ratio, especially in cryogenic setups.
Repeatability and reliability of low-temperature measurements.
To ensure bond integrity, I routinely perform:
Visual inspection under a microscope – to check bond placement, loop height, and adhesion.
Resistance measurement across bonded leads – to verify low-resistance connections.
Occasional pull testing – to assess mechanical stability when needed.
Repair & Troubleshooting Experience
I also have practical experience in maintaining and troubleshooting bonding equipment. Notably, I successfully repaired a TPT wire bonder, diagnosing and fixing issues in the force cylinder and motherboard. This helped restore full functionality and minimized experimental downtime.
When Wire Bonding Fails — Critical Factors
Even with a good tool and process, achieving a perfect bond can be challenging. Based on my hands-on experience, here are the key factors that can cause bonding failure:
Surface Contamination
Oxidized or dirty bond pads (from dust, resist residue, or environmental exposure) prevent proper wire adhesion.
Even minor contamination can drastically increase contact resistance.
Improper Tool Settings
Incorrect force, ultrasonic power, or bonding time can lead to weak or lifted bonds.
Different substrates and wire types require specific tuning.
Poor Alignment or Pad Geometry
Small or uneven pads (common in nano-devices or exfoliated flakes) make accurate bonding more difficult.
Misalignment can result in the wire not bonding at all or shorting adjacent features.
Inadequate Wire Looping or Tail Length
Loops that are too short or too long can break during cooling (especially in cryogenic setups).
Poor looping can also introduce mechanical strain on small substrates.
Tool Condition and Wear
A worn or misaligned capillary can result in consistent bonding issues.
I have diagnosed such issues in our lab and even repaired a TPT bonder, fixing the force cylinder and motherboard to restore optimal bonding performance.
Wire bonding may seem like a standard tool, but in cutting-edge spintronics — where device features are tiny, substrates are fragile, and measurements are highly sensitive — mastering it is critical. My experience spans not just routine bonding, but also process optimization, troubleshooting, and equipment repair, ensuring that my devices are measurement-ready with reliable electrical contacts.
J&K India, December 28, 2024
Punjab, India, March 21, 2025
Punjab, India, March 21, 2025
Bressanone/Brixen Italy, February 10, 2025
March 28, 2025