Subhadeep Datta’s research while affiliated with Jadavpur University and other places

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Publications (40)


FIG. 1. Schematic of growth setup and characterization of as-grown Te/MoS 2 heterostructures. (a) Schematic of CVD setup for the growth of MoS 2 . (b) SEM image of CVD-grown MoS 2 . (c) Schematic of PVD setup for the growth of Te NWs on MoS 2 -grown substrate. (d) SEM image of Te/MOs 2 heterostructure. (e) Raman spectra of Te, MoS 2 , and overlapping areas in the heterostructure. The brown line shows the Raman spectrum of Te NW, the gray line corresponds to the overlapping region, and the red line shows that of pristine MoS 2 . The inset shows an upshift of both characteristic Raman peaks in overlapped MoS 2 compared to pristine MoS 2 . (f) Photoluminescence spectra of monolayer MoS 2 from the pristine flake region (red) and the heterojunction region (gray). (g) Mapping of the surface potential of the heterostructure using KPFM to obtain the work function of the Te NW (brown line-cut), MoS 2 (red line-cut), and overlapping region (gray line-cut).
FIG. 2. Electrical transport measurements on SiO 2 . (a) False-colored SEM image of a tasted device fabricated by electron beam lithography (EBL). (b) Schematic of mixed-channel diode device. (c) Plots of I -V curves at different gate voltages measured across the p-n heterojunction device as shown in the schematic in panel (b) (drain at Te NW, source at MoS 2 ). The inset shows the rectification ratio at different gate voltages. (d) Transfer characteristics of p-n heterojunction FET at V DS = 3 V at different temperatures. (e) Schematic representation of the CAFM setup used for lateral transport measurements across the Te/MoS 2 heterostructure. Voltage sweeps from 0 up to ±10 V were applied to the tip while grounding the MoS 2 , and the current through the sample was simultaneously measured. The I -V measurements were carried out with 20 nA current compliance. (f) Semilog plot of current-voltage characteristic measured by CAFM across the Te NW (brown) and the heterojunction (gray).
FIG. 4. (a) Schematic of an SiO 2 -gated Te NW and MoS 2 FET. (b) Transconductance curve of Te NW (brown) at V DS = 0.1 V and MoS 2 (red) at V DS = 0.5 V with a SiO 2 back gate. (c) Schematic of an IL-top-gated Te NW and MoS 2 FET. (d) ILgated transconductance curves of Te NW (brown) at V DS = 0.1 V and MoS 2 (red) at V DS = 0.5 V. (e),(f) I -V characteristics of MoS 2 and Te devices measured at different IL-gate voltages, respectively. (g) Circuit diagrams of unipolar logic gates (Schmitt trigger) of Te NW (brown) and MoS 2 (red) with series load resistances (R L = 10 M). (h) Output curves of Schmitt-trigger devices (Te: brown, MoS 2 : red) at applied V DD = 0.4 V.
Tailored one-dimensional/two-dimensional van der Waals heterostructures for unified analog and digital electronics
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May 2025

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65 Reads

Physical Review Applied

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Shibnath Mandal

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Subhadeep Datta

We report a sequential two-step vapor deposition process for growing mixed-dimensional vdW materials, specifically Te nanowires (1D) and MoS2 (2D), on a single SiO2 wafer. Our growth technique offers a unique potential pathway to create large-scale, high-quality, defect-free interfaces. The assembled samples serve a twofold purpose: first, the as-prepared heterostructures (Te NW/MoS2) provide insights into the atomically thin depletion region of a 1D/2D vdW diode, as revealed by electrical transport measurements and density-functional-theory-based quantum transport calculations. The charge transfer at the heterointerface is confirmed using Raman spectroscopy and Kelvin probe force microscopy. We also observe modulation of the rectification ratio with varying applied gate voltage. Second, the nonhybrid regions on the substrate, consisting of the as-grown individual Te nanowires and MoS2 microstructures, are used to fabricate separate p- and n-type field-effect transistors (FETs), respectively. Furthermore, the ionic-liquid gating helps to realize a low-power complementary metal-oxide semiconductor (CMOS) inverter and all basic logic-gate operations using a pair of n- and p-FETs on the Si/SiO2 platform. This approach also demonstrates the potential for unifying diode and CMOS circuits on a single platform, opening opportunities for integrated analog and digital electronics.

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Ultrasound Tip‐Assisted Piezotronic Transduction in Monolayer MoS2

The interaction of ultrasonic waves with piezoelectric materials provides a quantitative route to enhance electrical and mechanical coupling in van der Waals (vdW) heterostructures. Here, wire‐bonding tip‐assisted ultrasound (≈100 kHz) is presented as an effective approach to achieve piezoelectric transduction in monolayer MoS2 on Si/SiO2 substrates. Transient current measurements show reproducible sharp peaks with a peak‐to‐base ratio (Ipeak/Ibase ≈ 12) unique to monolayer MoS2, under an impact duration of 10–100 ms. Electrostatic gate voltage (Vg) and ultrasound power (WP) tunable piezocurrent exhibit 3–5 times higher sensitivity in the ON‐state (Vg ⩾ 0) compared to the OFF‐state. Multiple reflections of acoustic waves at source‐drain electrodes, with an increment in reflection coefficients, enhance the linewidth of peak currents, validated by microacoustic simulations of surface acoustic wave (SAW) propagation in submicron geometries. The localized strain and Joule heating under ultrasonic excitation may generate a temperature rise of ≈20 K, which reduces activation energy barriers, potentially enhancing reaction rates in temperature‐sensitive chemical processes, such as hydrogen peroxide decomposition. This thermal‐damage‐free method integrates with silicon‐based fabrication, establishing a robust platform for on‐chip catalysis and energy harvesting in FET‐based piezotransducers.


FIG. 1. (a) Schematic representation of electron drag mediated by magnons in the FLG-FePS 3 heterostructure in the presence of an out-of-plane magnetic field (H ). An electric field (E ) is applied to the FLG layer to produce an electric current ( j) along its direction. The itinerant electrons in the FLG layer interact with the antiferromagnetic magnons at the interface, resulting in electronmagnon coupling via electrostatic interaction. Momentum transfer from the magnons to the electrons assists in their movement along the direction of the electric field, leading to an additional current ( j em ). (b) Schematic representation of out-of-plane capacitance measurement in the FLG-FePS 3 -FLG device in the presence of a DC bias (V dc ) and magnetic field (H ). Interfacial polarization develops between the surface-terminated charges of FePS 3 and the carriers in the FLG at the interfaces, as indicated by the dotted ellipses. The electrons, coupled with magnons, are represented with a spin, as the scattering event flips the spin states to conserve total angular momentum. The electron-magnon coupling influences the interfacial polarization and capacitance.
FIG. 2. Raman spectroscopy of (a) FLG/FePS 3 heterostructure (HS-1) at room temperature, obtained with an excitation wavelength of 473 nm. The spin-phonon coupled peaks are labeled as SP1-SP3. The emergence of distinct phonon modes from both FLG and FePS 3 in the FLG/FePS 3 heterostructure indicates the formation of a hetero-interface. The inset shows the appearance of three zone-folded phonon modes (ZPs) and a magnon mode (M) at low temperatures, which are not observed at room temperature. (b) The temperature-dependent spin-phonon coupled mode (∼250 cm −1 ) is plotted for isolated FePS 3 and the FLG/FePS 3 heterostructure (HS-1). The characteristic Néel temperature remains invariant (∼120 K) for both samples. The deviation from anharmonicity, ω, increases by more than three times in the heterostructure compared to the isolated flake.
FIG. 4. Normalized magnon stiffness (D ) and relative magnon frequency (ω) as functions of temperature in HS-1. The relative magnon frequency is calculated by subtracting all frequencies from the highest frequency value. In HS-1, the relative magnon frequency increases with temperature, while D also increases with temperature and remains within the shaded region. For comparison, the magnon stiffness of bcc iron is plotted at two different temperatures alongside our normalized stiffness values.
FIG. 5. Temperature dependence of change in capacitance with the applied magnetic field below T N . The change in capacitance increases at significantly lower temperatures than T N , from which magnon modes become prominent. Inset shows capacitance with applied DC voltage on a FLG/FePS 3 /FLG device measured at 100 kHz frequency at 50 K temperature with and without applying magnetic fields perpendicular to the ab plane. Upon the application of magnetic fields, the overall capacitance has been decreased. In the presence of magnetic fields, no significant changes have been observed in the trend of capacitance with the applied DC bias.
Electron-magnon coupling mediated magnetotransport in antiferromagnetic van der Waals heterostructures

April 2025

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91 Reads

Physical Review B

Magnons — wavelike spin excitations in magnets — transfer energy and information without moving charge, like ripples on water. Here, in FePS3, an antiferromagnetic insulator, magnons interact with the electrons of few-layer graphene when in a heterostructure, enabling spin waves to convert into electrical signals. In FePS3, magnons soften below 40 K, reducing stiffness with cooling, while few-layer graphene exhibits negative magnetoresistance at low fields (±0.2 T) up to 100 K, transitioning to positive beyond this point. This experiment also proposes a “magnon capacitor”, where spin waves regulate charge transport by influencing carrier dynamics at the interface. With possible applications in energy-efficient computing, this breakthrough advances next-generation spintronic technologies.


Magnetodielectric properties in two dimensional magnetic insulators

Magnetodielectric (MD) materials are important for their ability to spin-charge conversion, magnetic field control of electric polarization and vice versa. Among these, two-dimensional (2D) van der Waals (vdW) magnetic materials are of particular interest due to the presence of magnetic anisotropy (MA) originating from the interaction between the magnetic moments and the crystal field. Also, these materials indicate a high degree of stability in the long-range spin order and may be described using suitable spin Hamiltonians of the Heisenberg, XY, or Ising type. Recent reports have suggested effective interactions between magnetization and electric polarization in 2D magnets. However, MD coupling studies on layered magnetic materials are still few. This review covers the fundamentals of MD coupling by explaining related key terms. It includes the necessary conditions for having this coupling and sheds light on the possible microscopic mechanisms behind this coupling starting from phenomenological descriptions. Apart from that, this review classifies 2D magnetic materials into several categories for reaching out each and every class of materials. Additionally, this review summarizes recent advancements of some pioneer 2D MD materials. Last but not the least, the current review provides possible research directions for enhancing MD coupling in those and mentions the possibilities for future developments.


Magnetodielectric Properties in Two Dimensional Magnetic Insulators

February 2025

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15 Reads

Magnetodielectric (MD) materials are important for their ability to spin-charge conversion, magnetic field control of electric polarization and vice versa. Among these, two-dimensional (2D) van der Waals (vdW) magnetic materials are of particular interest due to the presence of magnetic anisotropy (MA) originating from the interaction between the magnetic moments and the crystal field. Also, these materials indicate a high degree of stability in the long-range spin order and may be described using suitable spin Hamiltonians of the Heisenberg, XY, or Ising type. Recent reports have suggested effective interactions between magnetization and electric polarization in 2D magnets. However, MD coupling studies on layered magnetic materials are still few. This review covers the fundamentals of magnetodielectric coupling by explaining related key terms. It includes the necessary conditions for having this coupling and sheds light on the possible physical mechanisms behind this coupling starting from phenomenological descriptions. Apart from that, this review classifies 2D magnetic materials into several categories for reaching out each and every class of materials. Additionally, this review summarizes recent advancements of some pioneer 2D magnetodielectric materials. Last but not the least, the current review provides possible research directions for enhancing magnetodielectric coupling in those and mentions the possibilities for future developments.


Raman signatures of inversion symmetry breaking structural transition in quasi-1D compound, (TaSe4)3I

January 2025

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40 Reads

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1 Citation

The breaking of inversion symmetry combined with spin–orbit coupling, can give rise to intriguing quantum phases and collective excitations. Here, we report systematic temperature dependent Raman scattering and theoretical calculations of phonon modes across the inversion symmetry-breaking structural transitions in a quasi-one-dimensional compound (TaSe4)3I. Our investigation revealed the emergence of three additional Raman-active modes in Raman spectra of the low-temperature non-centrosymmetric (NC) structure of the material. From polarization dependent Raman spectra and phonon mode symmetry analysis, we have identified the origin of these three newly appeared additional Raman-active modes. Notably, two of these modes become Raman active due to the loss of inversion symmetry, while the third mode is identified as a soft phonon mode, arising from the distinctive vibrational motion of tantalum (Ta) atoms along the –Ta–Ta– chains. Furthermore, the temperature evolution of self-energy parameters indicates significant changes in the characteristics of the Raman modes across the transition. Latent heat measurements near the phase transition using Differential Scanning Calorimetry confirm the first-order nature of the transition. Theoretical analysis, including group theory and modeling, reaffirms the displacive first-order nature of the structural transition. Our findings establish (TaSe4)3I as a model quasi-one-dimensional system with broken inversion symmetry facilitated through a displacive first-order structural transition.


Dimensional Crossover and Emergence of Novel Phases in Puckered PdSe2_2 under Pressure

January 2025

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46 Reads

We investigate the pressure-driven structural and electronic evolution of PdSe2_2 using powder X-ray diffraction, Raman spectroscopy, and first-principles calculations. Beyond 2.3 GPa, suppression of the Jahn-Teller distortion induces in-plane lattice expansion and metallization. Around 4.8 GPa, the interlayer dz2πd_{z^2}-\pi^* orbital hybridization drives the dimensional crossover, facilitating the transformation from the 2D distorted to a 3D undistorted pyrite phase. Above 9 GPa, a novel phase emerges, characterized by octahedral distortions in the d orbitals of Pd. Structural analysis suggests the presence of marcasite (Pnnm) or arsenopyrite (P21/cP2_1/c) phase with orthorhombic and monoclinic configurations, respectively. Furthermore, the observed phonon anomaly and electronic structure modifications, including the emergence of flat bands in the high-pressure phases, elucidate the fundamental mechanisms underlying the previously reported exotic superconductivity with an enhanced critical temperature. These results highlight the pivotal role of dimensional crossover and structural transitions in tuning the electronic properties of puckered materials, providing pathways for novel functionalities.


FIGURE 2. (a) Magnetic structure of a single layer of Fe 2+ ions in FePS3. The black filled circles represent spins pointing out of the plane of the paper, while the white hollow circles represent spins pointing into the plane of the paper. Two of the nearest neighbors are ferromagnetically coupled, whereas the third is coupled antiferromagnetically. The two crystallographically inequivalent sites are labelled as A and B. For a A-type site, the nearest neighbor bonds are given by the vectors, í µí»¿ 1 ⃗⃗⃗ = í µí±Ž (− √3 2 í µí±¥ ̂ − 1 2 í µí±¦ ̂), í µí»¿ 2 ⃗⃗⃗ = í µí±Ž ( √3 2 í µí±¥ ̂ − 1 2 í µí±¦ ̂), and í µí»¿ 3 ⃗⃗⃗ = í µí±Ží µí±¦ ̂, where í µí±Ž is the lattice constant. The magnetic field ℎ ⃗ points out of the plane of the paper. (b) The structure can be interpreted to made up of 4 interpenetrating magnetic sublattices. Inset: The first magnetic Brillouin zone (in red) and the first crystallographic Brillouin zone (in black). (c) Comparison of theoretical results (continuous lines) and experimental results (dots) for the variation of the energy bands with the applied field. Fitted parameters are given in the text. (d) shows a zoomed-in portion of (c), with the different magnon and phonon branches marked.
Magnon-Phonon Coupling in Layered Antiferromagnet

December 2024

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49 Reads

We present a fully analytical model of hybridization between magnon, and phonons observed experimentally in magneto-Raman scattering in van der Waals (vdW) antiferromagnets (AFM). Here, the representative material, FePS3, has been shown to be a quasi-two-dimensional-Ising antiferromagnet, with additional features of spin-phonon coupling in the Raman spectra emerging below the N\'eel temperature (TN) of approximately 120 K. Using magneto-Raman spectroscopy as an optical probe of magnetic structure, we show that one of these Raman-active modes in the magnetically ordered state is a magnon with a frequency of 3.7 THz (~ 122 cm-1). In addition, one magnon band and three phonon bands are coupled via the magneto-elastic coupling evidenced by anti-crossing in the complete spectra. We consider a simple model involving only in-plane nearest neighbor exchange couplings (designed to give rise to a similar magnetic structure) and perpendicular anisotropy in presence of an out-of-plane magnetic field. Exact diagonalization of the Hamiltonian leads to energy bands which show that the interaction term gives rise to avoided crossings between the hybridized magnon and phonon branches. Realizing magnon-phonon coupling in two-dimensional (2D) AFMs is important for the verification of the theoretical predictions on exotic quantum transport phenomena like spin-caloritronics, topological magnonics, etc.


Tailored 1D/2D Van der Waals Heterostructures for Unified Analog and Digital Electronics

December 2024

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47 Reads

We report a sequential two-step vapor deposition process for growing mixed-dimensional van der Waals (vdW) materials, specifically Te nanowires (1D) and MoS2_2 (2D), on a single SiO2_2 wafer. Our growth technique offers a unique potential pathway to create large scale, high-quality, defect-free interfaces. The assembly of samples serves a twofold application: first, the as-prepared heterostructures (Te NW/MoS2_2) provide insights into the atomically thin depletion region of a 1D/2D vdW diode, as revealed by electrical transport measurements and density functional theory-based quantum transport calculations. The charge transfer at the heterointerface is confirmed using Raman spectroscopy and Kelvin probe force microscopy (KPFM). We also observe modulation of the rectification ratio with varying applied gate voltage. Second, the non-hybrid regions on the substrate, consisting of the as-grown individual Te nanowires and MoS2_2 microstructures, are utilized to fabricate separate p- and n-FETs, respectively. Furthermore, the ionic liquid gating helps to realize low-power CMOS inverter and all basic logic gate operations using a pair of n- and p- field-effect transistors (FETs) on Si/SiO2_2 platform. This approach also demonstrates the potential for unifying diode and CMOS circuits on a single platform, opening opportunities for integrated analog and digital electronics.



Citations (17)


... Raman spectroscopy serves as a powerful tool for investigating phase transitions and various elementary excitations, including lattice vibrations, electron-phonon interactions, and spin-phonon interactions, particularly in reduced dimensions [34,35]. To explore the antiferromagnetic (AFM) properties of MnSe and establish the correlation between spin dynamics and phonon modes, we conducted temperature-dependent Raman spectroscopy measurements. ...

Reference:

Revisiting MnSe : a Magnetic Semiconductor with Spin-Phonon coupling
Raman signatures of inversion symmetry breaking structural transition in quasi-1D compound, (TaSe4)3I

... 1,17 This suggests either the presence of an intrinsic easy-plane magnetocrystalline anisotropy or that the magnetisation is inhomogeneous across the vdW layers and gaps, leading to a stronger shape anisotropy than expected from the measured M s . 1 The g-factor obtained from the BLS measurements (see Methods) consistently falls in the range g = 2.1 − 2.3, showing no significant temperature dependence, in close agreement with previous reports. 1,21 The notable deviation from the freeelectron value of g = 2.0 suggests a substantial orbital moment and significant spin-orbit coupling in the material. This is consistent with the orbital/spin moment ratio measured in. ...

Room Temperature Evolution of Laser‐Induced Ultrafast Spin and Phonon Dynamics in 2D van der Waals Magnets FexGeTe2 (x = 3, 4, 5)

... [32][33][34][35][36]. Heterostructures of FLG and FePS 3 are fabricated by placing FePS 3 on top of FLG using a micromanipulator (see the Supplemental Material [37], Sec. I, for details of the transfer process) and they are denoted as [32,[38][39][40]. The thickness and the quality of the heterostructure interfaces were confirmed by atomic force microscopy in the tapping and conducting mode (Asylum Research MFP-3D) (see Supplemental Material [37], Figs. ...

Pressure-induced insulator-to-metal transition in few-layer FePS 3 at 1.5 GPa
  • Citing Article
  • June 2024

... Bulk GeS has an indirect bandgap of approximately 1.6 eV, like that of other materials like MoS₂ (1.3 eV for bulk) and WS₂ (1.4 eV for bulk), which also exhibit indirect bandgaps [6][7][8]. In contrast, the monolayer form of GeS retains an indirect bandgap of about 1.95 eV, unlike monolayer MoS₂ (1.8 eV) and WS₂ (2.0 eV), which transition to a direct bandgap. ...

Unraveling electronic structure of GeS through ARPES and its correlation with anisotropic optical and transport behavior

... The local magnetic moments generated by these vacancies are estimated as 3.3m B per vacancy based on our DFT calculations and the literature. [44][45][46][47][48][49][50][51] Fig. 4c depicts the spin orientation in the heterostructure under a downward magnetic field. The reversal of magnetic moment alignment in Pt, induced by the downward field, demonstrates the effective moments of vacancies and the switchable polarity of the MPE in response to an external field. ...

Manipulating Spin‐Lattice Coupling in Layered Magnetic Topological Insulator Heterostructure via Interface Engineering

... 2D LaOCl have emerged as a promising layered highκ dielectric according to density functional theory [184]. This suggests significant potential for its application in transistors [185,186]. Looking ahead, the exploration of magnetic properties in these 2D RE materials could unlock new opportunities in developing advanced magnetic devices and technologies. ...

Negative Capacitance for Stabilizing the Logic State in a Tunnel Field-Effect Transistor
  • Citing Article
  • April 2024

ACS Applied Nano Materials

... While magnon stiffness can be measured by inelastic neutron scattering (INS), measuring the same in the HS framework is beyond the scope of our study. In pristine FePS 3 (T N ∼ 120 K), magnetization and magnon stiffness both increase with cooling below 60 K [11,59]. However, in the FLG/FePS 3 HS, the magnon mode softens below 70 K (see Supplemental Material [37], Fig. SXI), suggesting weakened magnetization and possible restoration of the antiferromagnetic ground state [59]. ...

Anisotropic magnetodielectric coupling in layered antiferromagnetic FePS 3

... Room-temperature current-voltage (I -V) measurements were also performed using CAFM, with Ti/Au and Au serving as the contacts to MoS 2 and the Te NW, respectively [53][54][55][56], as indicated in Fig. 2(e). A conducting tip was used to measure the local current at different positions of the individual semiconductors and heterostructures. ...

Ultrahigh breakdown current density of van der Waals one dimensional PdBr2
  • Citing Article
  • June 2023

... Pd, Pt and X: chalcogenides e.g. S, Se, Te) which can be tuned to a variety of polymorphs under external perturbation (pressure, temperature, etc.) or chemical intercalation [2][3][4][5]. As a viable tuning parameter, pressure plays a crucial role in altering the crystal structure as well as band structure without introducing any chemical disorder. ...

Tunable Electron Transport in Defect-Engineered PdSe 2
  • Citing Article
  • June 2023

Chemistry of Materials

... The value of 0 is found to be small but positive [13,66]. The C in F3GT-2 is little higher than F3GT-1 due to the multiple magnetic phases that can be attributed to the change in nearest neighbor Fe-Fe distance with the development of a secondary phase of FeTe [67]. ...

Emergence of a Non‐Van der Waals Magnetic Phase in a Van der Waals Ferromagnet