| Temperature (K) | Emission peak (eV/nm) | FWHM (eV) | ho (cm-1) | Intensity (a.u.) | I 1/I 2 |
| 20              | 2.655/467.0           | 0.371     | 1050      | 406.3            | 1.03    |
|                 | 2.842/436.3           | 0.233     | 1098      | 396.4            | 1.03    |
|                 |                       |           |           |                  |         |
| 70              | 2.664/465.5           | 0.372     | 1206      | 362.4            | 1.03    |
|                 | 2.849/435.2           | 0.235     | 1242      | 353.0            | 1.03    |
|                 |                       |           |           |                  |         |
| 140             | 2.652/467.6           | 0.373     | 1212      | 310.8            | 0.92    |
|                 | 2.843/436.2           | 0.240     | 1283      | 338.3            | 0.92    |
|                 |                       |           |           |                  |         |
| 300             | 2.646/468.6           | 0.380     | 1450      | 205.8            | 0.90    |
|                 | 2.830/438.2           | 0.247     | 1495      | 228.8            | 0.90    |

Caption: Gaussian fitting results of emission spectra for stilbene-3 doped lead-tin-fluorophosphate glass excited by 320nm at different temperatures, including emission peak, FWHM (full width at half maximum), phonon energies ho, integrated intensity, and ratio of intensity of two bands

You are provided with a table from a material science paper. Here are JSON templates for two types of numeric cells: "Other" and "Glass_Compound_Amount":
{"value": "xx", "type": "Other"}
{"value": "xx", "type": "Glass_Compound_Amount", "constituent": "xx", "unit": "xx", "material": "xx"}

Please describe all numeric cells in the above table following the JSON templates (proceeding by row in a left-right, top-down direction). For each cell, output one JSON description per line. For any unanswerable attributes in the templates, set their value to the placeholder "xx".

Cell Description:
{"value": "20", "type": "Other"}
{"value": "2.655", "type": "Other"}
{"value": "467.0", "type": "Other"}
{"value": "0.371", "type": "Other"}
{"value": "1050", "type": "Other"}
{"value": "406.3", "type": "Other"}
{"value": "1.03", "type": "Other"}
{"value": "2.842", "type": "Other"}
{"value": "436.3", "type": "Other"}
{"value": "0.233", "type": "Other"}
{"value": "1098", "type": "Other"}
{"value": "396.4", "type": "Other"}
{"value": "1.03", "type": "Other"}
{"value": "70", "type": "Other"}
{"value": "2.664", "type": "Other"}
{"value": "465.5", "type": "Other"}
{"value": "0.372", "type": "Other"}
{"value": "1206", "type": "Other"}
{"value": "362.4", "type": "Other"}
{"value": "1.03", "type": "Other"}
{"value": "2.849", "type": "Other"}
{"value": "435.2", "type": "Other"}
{"value": "0.235", "type": "Other"}
{"value": "1242", "type": "Other"}
{"value": "353.0", "type": "Other"}
{"value": "1.03", "type": "Other"}
{"value": "140", "type": "Other"}
{"value": "2.652", "type": "Other"}
{"value": "467.6", "type": "Other"}
{"value": "0.373", "type": "Other"}
{"value": "1212", "type": "Other"}
{"value": "310.8", "type": "Other"}
{"value": "0.92", "type": "Other"}
{"value": "2.843", "type": "Other"}
{"value": "436.2", "type": "Other"}
{"value": "0.240", "type": "Other"}
{"value": "1283", "type": "Other"}
{"value": "338.3", "type": "Other"}
{"value": "0.92", "type": "Other"}
{"value": "300", "type": "Other"}
{"value": "2.646", "type": "Other"}
{"value": "468.6", "type": "Other"}
{"value": "0.380", "type": "Other"}
{"value": "1450", "type": "Other"}
{"value": "205.8", "type": "Other"}
{"value": "0.90", "type": "Other"}
{"value": "2.830", "type": "Other"}
{"value": "438.2", "type": "Other"}
{"value": "0.247", "type": "Other"}
{"value": "1495", "type": "Other"}
{"value": "228.8", "type": "Other"}
{"value": "0.90", "type": "Other"}