|                 | T  m  [K] | T  d  [K] | e(T  d ) | T  g  [K] | e(T  g ) | log    e   T g     e   T d |
| PS [11]         | 1037      | 775       | 2.97106  | 683       | 2.71011  | 4.959                      |
| L2B [22]        | 1190      | 795       | 2.20108  | 768       | 2.091011 | 2.979                      |
| L3S [11]        | 1306      | 953       | 5.36106  | 734       | 1.451012 | 5.433                      |
| L2S [13]        | 1307      | 809       | 1.33108  | 727       | 7.331011 | 3.742                      |
| Li-7.5 [19]     | 1435      | 788       | 1.28109  | 748       | 5.691011 | 2.648                      |
| N1C3S [32]      | 1469      | 830       | 4.71106  | 743       | 8.461011 | 5.255                      |
| Li-0 [19]       | 1564      | 907       | 9.40108  | 838       | 2.491012 | 3.422                      |
| Cordierite [11] | 1643      | 1192      | 2.47108  | 1083      | 3.91012  | 4.198                      |
| Diopside [11]   | 1664      | 1072      | 1.17108  | 995       | 9.21011  | 3.894                      |
| B2S [33]        | 1693      | 1016      | 3.20109  | 961       | 1.681012 | 2.721                      |
| Fresnoite [35]  | 1714      | 1009      | 1.101010 | 983       | 8.71011  | 1.896                      |

Caption: Melting (T m ), decoupling (T d ), and glass transition (T g ) temperatures, viscosities at T d and T g , and ratios of the viscosities at these temperatures for a set of liquids. The glass transition temperature refers to a good approximation (cf. Fig. 7) to a viscosity e(T g )1012Pas, i.e., the glass transition temperature refers widely to the value one obtains according to Tammann's definition of T g . The following systems are analyzed: PbO*SiO2 (PS), Li2O*2B2O3 (L2B), Li2O*3SiO2 (L3S), Li2O*2SiO2 (L2S), Na2O*2CaO*3SiO2-Li2O (Li-7.5), 2Na2O*1Cao*3SiO2 (2N1C3S), Na2O*2CaO*3SiO2 (Li-0), cordierite, CaO*MgO*2SiO2 (diopside), BaO*2SiO2 (B2S), and Ba2Ti(Si2O7)O (fresnoite).

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": "1037", "type": "Other"}
{"value": "775", "type": "Other"}
{"value": "2.97106", "type": "Other"}
{"value": "683", "type": "Other"}
{"value": "2.71011", "type": "Other"}
{"value": "4.959", "type": "Other"}
{"value": "1190", "type": "Other"}
{"value": "795", "type": "Other"}
{"value": "2.20108", "type": "Other"}
{"value": "768", "type": "Other"}
{"value": "2.091011", "type": "Other"}
{"value": "2.979", "type": "Other"}
{"value": "1306", "type": "Other"}
{"value": "953", "type": "Other"}
{"value": "5.36106", "type": "Other"}
{"value": "734", "type": "Other"}
{"value": "1.451012", "type": "Other"}
{"value": "5.433", "type": "Other"}
{"value": "1307", "type": "Other"}
{"value": "809", "type": "Other"}
{"value": "1.33108", "type": "Other"}
{"value": "727", "type": "Other"}
{"value": "7.331011", "type": "Other"}
{"value": "3.742", "type": "Other"}
{"value": "1435", "type": "Other"}
{"value": "788", "type": "Other"}
{"value": "1.28109", "type": "Other"}
{"value": "748", "type": "Other"}
{"value": "5.691011", "type": "Other"}
{"value": "2.648", "type": "Other"}
{"value": "1469", "type": "Other"}
{"value": "830", "type": "Other"}
{"value": "4.71106", "type": "Other"}
{"value": "743", "type": "Other"}
{"value": "8.461011", "type": "Other"}
{"value": "5.255", "type": "Other"}
{"value": "1564", "type": "Other"}
{"value": "907", "type": "Other"}
{"value": "9.40108", "type": "Other"}
{"value": "838", "type": "Other"}
{"value": "2.491012", "type": "Other"}
{"value": "3.422", "type": "Other"}
{"value": "1643", "type": "Other"}
{"value": "1192", "type": "Other"}
{"value": "2.47108", "type": "Other"}
{"value": "1083", "type": "Other"}
{"value": "3.91012", "type": "Other"}
{"value": "4.198", "type": "Other"}
{"value": "1664", "type": "Other"}
{"value": "1072", "type": "Other"}
{"value": "1.17108", "type": "Other"}
{"value": "995", "type": "Other"}
{"value": "9.21011", "type": "Other"}
{"value": "3.894", "type": "Other"}
{"value": "1693", "type": "Other"}
{"value": "1016", "type": "Other"}
{"value": "3.20109", "type": "Other"}
{"value": "961", "type": "Other"}
{"value": "1.681012", "type": "Other"}
{"value": "2.721", "type": "Other"}
{"value": "1714", "type": "Other"}
{"value": "1009", "type": "Other"}
{"value": "1.101010", "type": "Other"}
{"value": "983", "type": "Other"}
{"value": "8.71011", "type": "Other"}
{"value": "1.896", "type": "Other"}