Future Works

5.1 Future Testing Using SEM and TEM

Due to time constraints and equipment downtime during the project period, the sidewall angle measurements obtained from electron detector analysis could not be independently verified against a direct cross-sectional technique. The error function and Gaussian edge fitting method used in this project provides an indirect estimate of θ inferred from the top-down intensity profile. It assumes that the feature geometry is the dominant contributor to the edge transition width f. Cross-sectional verification would either confirm or correct this assumption, and is strongly recommended for any future iteration of this work.

Direct Sidewall Imaging via Stage Tilt

A tilted SEM approach can provide a direct line-of-sight measurement of the sidewall profile without requiring sample destruction. The JEOL JSM-6700F specimen stage supports tilt angles of −5° to +60°, so that the sidewall of the grid feature is brought into a near-parallel view relative to the incident electron beam. The apparent width of the edge band in the tilted image can then be compared to the top-down measurement; the geometric relationship between the two gives an independent estimate of the sidewall angle.

sem tilt method
Figure 5.1: Simplified diagram of the SEM stage tilt

A more direct method is to cleave or FIB-mill the sample through a grid line and image the exposed cross-section. This gives a true side-on view of the feature profile, and the sidewall angle can be measured directly from the image by fitting a line to the sidewall edge.

TEM Cross-Sectional Verification

Transmission electron microscopy offers the highest spatial resolution for sidewall angle measurement and is the reference technique used by NIST for the SCCDRM single-crystal standards. The procedure involves thinning the sample down to electron transparency using FIB milling, progressively reducing the lamella to a thickness of a few tens of nanometres until the cross-section of the grid feature is exposed. At this thickness, the high-angle annular dark field (HAADF-STEM) mode provides direct imaging of the metal-resist and metal-silicon interfaces with sub-nanometre resolution, and the sidewall angle can be measured directly from the atomic-scale image of the metal column edge.

The primary limitation of TEM is that sample preparation is destructive and time-consuming. Each FIB-prepared lamella represents one measurement site on one sample, and the preparation process itself introduces artefacts at the cut surface. For this project, TEM verification would be most valuable on the best-performing sample identified from the SEM and AFM results, to establish a ground-truth measurement of θ against which the indirect error function estimates can be calibrated for future use.

5.2 Scalability via Nanoimprinting

Nanoimprint lithography (NIL) offers a path to high-throughput replication of the grid resolution standard without requiring repeated PBW exposures. In this approach, a PBW-fabricated PMMA master is used as a stamp to imprint the grid pattern into a fresh polymer substrate, transferring the geometry in a single press cycle.

Initial trials were conducted using an Omostamp silicon stamp on a NILT CNI nanoimprinter (software v1.0.0.42). The hot embossing recipe used is summarised in Table 5.1.

Nanoimprinting overview
Figure 5.2: Nanoimprinting process overview.

Table 5.1: Nanoimprint recipe parameters (NILT CNI, hot embossing)

Step Parameter Value
1: Vacuum Threshold 90.0
  ForceVac 0
  VacTime 0.2 min
2: Temperature ramp Target temperature 130 °C
  Ramp time 0.0 min
  Pressure 1.0 bar
  Wait for temp Yes
3: Hold Hold time 10.0 min
  Imprint pressure 9.0 bar
4: Cooldown ramp Target temperature 60 °C
  Pressure 9.0 bar
  Wait for temp Yes
Nanoimprinting machine
Figure 5.3: NILT CNI nanoimprinting machine.

Two problems were identified in the initial trials. First, the PMMA resist layer delaminated from the silicon wafer during demolding: the grid features were pulled off the substrate rather than transferring cleanly into the imprint polymer. This is likely caused by insufficient adhesion between the PMMA and the silicon surface, either due to inadequate surface preparation or wafer contamination prior to spin coating. Depositing a thin adhesion layer (e.g. HMDS or Cr) between the silicon and PMMA prior to PBW is a recommended corrective step.

Second, the PMMA film thickness exceeded the Omostamp feature height, causing overflow of resist material beyond the patterned region during the imprint step. Future trials should match the PMMA spin thickness more closely to the stamp feature height, either by reducing the spin-coated thickness or by selecting a lower-concentration PMMA grade.

Resolving these two issues would make NIL a viable route for producing multiple copies of the grid standard from a single PBW master, significantly reducing the cost and time per calibration artefact.

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