Skip to content

Nanofluidics of Single-Crystal Diamond Nanomechanical Resonators

MetadataDetails
Publication Date2015-10-28
JournalNano Letters
AuthorsVural Kara, Young-Ik Sohn, Haig A. Atikian, Victor Yakhot, Marko Lončar
InstitutionsBoston University, Harvard University
Citations30
AnalysisFull AI Review Included

Technical Analysis and Commercial Solutions: Nanofluidics of Single-crystal Diamond Nanomechanical Resonators

Section titled “Technical Analysis and Commercial Solutions: Nanofluidics of Single-crystal Diamond Nanomechanical Resonators”

This document analyzes the research paper, “Nanofluidics of Single-crystal Diamond Nanomechanical Resonators,” to extract key technical data and propose specific material solutions and engineering capabilities offered by 6CCVD.


  • Core Research Focus: Systematic study of single-crystal diamond (SCD) nanomechanical resonators (nanocantilevers) operating in fluids, specifically high-purity He, N2, Ar gases, and water.
  • Dissipation Scaling Mechanism: Conclusively demonstrated that the fluidic dissipation mechanism in gases is governed by a subtle interplay between the cantilever length scale (via the Knudsen number, Kn) and the resonance frequency (via the Weissenberg number, Wi).
  • Surface Accommodation: Achieved the first reported measurement of gas surface accommodation coefficients (K) on single-crystal diamond, showing that lighter gases (He) reflect more specularly than heavier gases (Ar and N2).
  • Material Performance: The SCD nanocantilevers exhibited extremely high vacuum quality factors (Q0 up to 1.7 x 105), confirming the low intrinsic dissipation necessary for high-sensitivity NEMS applications.
  • Liquid Characterization: Successfully measured thermal fluctuations and calculated frequency shifts and quality factors (Qw) in water, validating current hydrodynamic theory for the mass loading parameter (T0 ≈ 0.69).
  • Fabrication Challenge: The use of angled-etching resulted in non-ideal triangular cross-sections, introducing uncertainty in mass loading calculations (T0), highlighting the need for highly uniform material processing.

The following parameters were extracted directly from the experimental measurements and theoretical analysis presented in the paper.

ParameterValueUnitContext
SCD Film Thickness (h)0.530”mTypical dimension for cantilevers studied
SCD Cantilever Width (w)0.820”mTypical dimension for cantilevers studied
Length Range (l)4.8 to 48”mRange of nanocantilevers fabricated and tested
Vacuum Resonance Frequency (f0)0.411 to 40.032MHzFull frequency range of devices
Vacuum Quality Factor (Q0)1.5 x 104 to 1.7 x 105DimensionlessDemonstrates low intrinsic material dissipation
Atmosphere Quality Factor (Qatm)~ 102DimensionlessTypical Q in N2 at atmospheric pressure
Water Quality Factor (Qw)0.75 to 2.55DimensionlessHighly overdamped regime
Top Surface Roughness (r.m.s.)< 1nmAchieved by protection layer during etching
Sidewall Roughness (r.m.s.)≀ 10nmResulting from oxygen plasma angled-etch
N2 Transition Pressure (pc) Range44 ± 5 to 211 ± 11TorrPressure where flow transitions (molecular to viscous)
Mass Loading Parameter (T0)0.69 ± 0.1DimensionlessRatio of entrained fluid mass to solid mass in water
Accommodation Coefficient Ratio (K)KAr : KN2 : KHe ≈ 1 : 0.97 : 0.92DimensionlessMeasured ratio showing difference in gas reflection

The following process steps summarize the material fabrication, preparation, and experimental setup necessary to conduct the nanofluidic characterization:

  1. Material Growth: High-purity single-crystal diamond (SCD) films were utilized as the base material, exploiting their unique mechanical properties (high Young’s modulus, low intrinsic dissipation).
  2. Nanocantilever Fabrication: Devices were manufactured using a non-standard angled-etching technique involving a two-step etch process (vertical oxygen plasma followed by an oblique angle etch).
  3. Cross-Sectional Geometry: The angled-etch resulted in non-rectangular (triangular) cross-sections (approximately 820 nm x 530 nm), requiring post-facto confirmation via Focused Ion Beam (FIB) milling after coating with a few-micron-thick platinum layer.
  4. Surface Preparation & Quality: The top cantilever surface was protected, resulting in a low r.m.s. roughness (< 1 nm), while the etched sidewalls exhibited roughness up to 10 nm r.m.s.
  5. Gas Experimentation: Experiments used high-purity He, N2, and Ar gases in a custom-built vacuum chamber capable of pressures down to 10-7 Torr, measured using calibrated capacitive gauges.
  6. Liquid Experimentation: Thermal fluctuations of the resonators were measured in a small fluid chamber filled with water.
  7. Sensing Mechanism: Out-of-plane displacements were measured using a path-stabilized Michelson interferometer operating in the 1-50 MHz range, providing a displacement sensitivity of approximately 30 fm/√Hz.

6CCVD is positioned to supply the high-purity single-crystal diamond materials and specialized processing required to replicate and advance this crucial nanofluidics research, addressing the challenges of dimensional uncertainty and surface accommodation control.

To replicate the high Q0 values and investigate complex fluid dynamics, Optical Grade Single Crystal Diamond (SCD) is required.

6CCVD Material SolutionSpecificationsApplication Context
High-Purity SCD WafersThickness: 0.1 ”m to 500 ”m. Size: Up to 125 mm.Provides the ultra-low intrinsic dissipation base material necessary for high Q nanomechanical resonators.
Boron-Doped Diamond (BDD)Custom doping levels available (Heavy/Moderate).Ideal for extending the research into electrochemical nanofluidics or biosensing where surface functionalization is required.

The study noted geometric uncertainty due to the angled etch resulting in triangular cross-sections. 6CCVD’s capabilities eliminate this variance and support complex post-fabrication needs.

  • Precision Diamond Processing: 6CCVD provides SCD films with exceptional thickness uniformity, allowing researchers to use standard, uniform vertical plasma etching. This eliminates the non-rectangular cross-section issue, improving the accuracy of mass loading (T0) and dissipation models.
  • Custom Dimensions and Etch Preparation: We supply wafers and plates cut to custom specifications using internal laser cutting services, ensuring precise geometries and edge quality far superior to manual breaking or post-process FIB trimming.
  • Advanced Polishing for K-Coefficient Control: The study highlights the critical role of surface roughness (Ra < 1 nm) in controlling the gas accommodation coefficient (K). 6CCVD guarantees Ra < 1 nm polishing on SCD wafers, essential for repeatable, predictable molecular flow experiments. We also offer Ra < 5 nm polishing for inch-sized Polycrystalline Diamond (PCD) wafers for cost-sensitive applications.
  • Custom Metalization Schemes: The need for electrical contacts in advanced NEMS is standard. 6CCVD offers in-house deposition of thin-film metals, including Au, Pt, Pd, Ti, W, and Cu, crucial for integrating measurement electrodes or resistive heating elements into the nanocantilever devices.

6CCVD’s in-house expertise goes beyond material supply. We offer specialized consultation to overcome research hurdles.

  • Our in-house PhD team can assist researchers in material selection, focusing specifically on optimizing surface termination and purity necessary for controlling surface accommodation coefficients (K) in gas sensing projects.
  • We provide expert guidance on preparing substrates for complex nanofabrication techniques, ensuring material stability and maximizing yield for high-aspect-ratio structures like those used in this nanofluidic sensing project.
  • Global Logistics: All materials are shipped globally, DDU default with DDP options available, ensuring prompt delivery of highly specialized diamond products directly to your lab.

For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.

View Original Abstract

Single-crystal diamond nanomechanical resonators are being developed for countless applications. A number of these applications require that the resonator be operated in a fluid, that is, a gas or a liquid. Here, we investigate the fluid dynamics of single-crystal diamond nanomechanical resonators in the form of nanocantilevers. First, we measure the pressure-dependent dissipation of diamond nanocantilevers with different linear dimensions and frequencies in three gases, He, N2, and Ar. We observe that a subtle interplay between the length scale and the frequency governs the scaling of the fluidic dissipation. Second, we obtain a comparison of the surface accommodation of different gases on the diamond surface by analyzing the dissipation in the molecular flow regime. Finally, we measure the thermal fluctuations of the nanocantilevers in water and compare the observed dissipation and frequency shifts with theoretical predictions. These findings set the stage for developing diamond nanomechanical resonators operable in fluids.