Figures & data
Table 1. Material properties of copper and molybdenum.
Figure 2. Schematic representation of the arrangement of seed substrates on Molybdenum substrate holder.
![Figure 2. Schematic representation of the arrangement of seed substrates on Molybdenum substrate holder.](/cms/asset/92c37919-859a-4e42-b187-c28be6d1d973/tfdi_a_2350967_f0002_c.jpg)
Figure 6. Reported growth of single crystal diamond seeds after (a) 130 h (b) 9 mm× 9 mm × 1.85 mm cubes grown in 171 h process cycle using welding method.
![Figure 6. Reported growth of single crystal diamond seeds after (a) 130 h (b) 9 mm× 9 mm × 1.85 mm cubes grown in 171 h process cycle using welding method.](/cms/asset/998fe47d-c72f-4a00-86ea-2d953ceaecfe/tfdi_a_2350967_f0006_c.jpg)
Table 2. Summary of growth parameters.
Figure 7. Reported growths of single crystal diamond seeds after (a) 18 h (b) 25 h (c) 130 h using (d) 9 mm× 9 mm × 1.85 mm cubes grown in 154 h process cycle using welding method.
![Figure 7. Reported growths of single crystal diamond seeds after (a) 18 h (b) 25 h (c) 130 h using (d) 9 mm× 9 mm × 1.85 mm cubes grown in 154 h process cycle using welding method.](/cms/asset/cc82b6c2-2aa8-4705-80c6-c3bb20dac092/tfdi_a_2350967_f0007_c.jpg)
Table 3. Temperature distribution of conventional method for different process cycle.
Table 4. Temperature distribution of welding method for different process cycle.
Figure 9. Raman Spectra taken from the samples; Excitation laser wavelength is 532 nm (a) for S1 sample grown using the conventional method (b) for S2 grown using welding method.
![Figure 9. Raman Spectra taken from the samples; Excitation laser wavelength is 532 nm (a) for S1 sample grown using the conventional method (b) for S2 grown using welding method.](/cms/asset/d568423b-69d7-4289-8edd-9b7cb100e8aa/tfdi_a_2350967_f0009_b.jpg)
Figure 10. (a) The transmittance spectrum shows maximum transmission at 1336 nm of S1 and (b) Absorbance spectrum shows peak at 220 nm of sample S1.
![Figure 10. (a) The transmittance spectrum shows maximum transmission at 1336 nm of S1 and (b) Absorbance spectrum shows peak at 220 nm of sample S1.](/cms/asset/cbb3a076-b607-4b51-a84f-8574708b7c0b/tfdi_a_2350967_f0010_b.jpg)
Figure 11. (a) Transmittance spectrum shows maximum transmission at 412 nm of S2 and (b) Absorbance spectrum shows a peak at 282 nm of sample S2.
![Figure 11. (a) Transmittance spectrum shows maximum transmission at 412 nm of S2 and (b) Absorbance spectrum shows a peak at 282 nm of sample S2.](/cms/asset/f6a6c2bc-39ff-4a3f-bdcc-d23aa4516016/tfdi_a_2350967_f0011_b.jpg)
Figure 12. (a) Absorption coefficient spectra shows a peak at 220 nm (b) Absorption coefficient spectra shows zero phonon line at 502 nm of sample S1.
![Figure 12. (a) Absorption coefficient spectra shows a peak at 220 nm (b) Absorption coefficient spectra shows zero phonon line at 502 nm of sample S1.](/cms/asset/b668b1d1-aff7-49b6-8d41-b78904ed69e8/tfdi_a_2350967_f0012_b.jpg)
Figure 13. (a) Absorption coefficient spectra shows a peak at 280 nm (b) Absorption coefficient spectra shows zero phonon line at 502 nm of sample S2.
![Figure 13. (a) Absorption coefficient spectra shows a peak at 280 nm (b) Absorption coefficient spectra shows zero phonon line at 502 nm of sample S2.](/cms/asset/1e7cb0da-eb85-4159-ab8d-ca03c9061ff9/tfdi_a_2350967_f0013_b.jpg)