lithium niobate / Data / coercive-field-ratio-cln-sln

Coercive field ratio Ec(CLN)/Ec(SLN)

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one row per variant and wavelength

Each mark is one record; bars are stated ranges, whiskers stated uncertainties. Filled marks: P, P-comp, P-db; hollow: S, V, C, P(abs). Hover a mark for its source. Each row has its own axis; no mean or fit is drawn.

Records

1 variant

Value	Unit	Variant	Conditions	Frame	Source	Locator	Status
≈ 4 to 5	–	Congruent LiNbO3 (CLN) CLN (C = 0.484) vs near-SLN (C = 0.498)	T room temperature	–	Gopalan et al., Applied Physics Letters 72 1981 (1998)	abstract	P(abs)
3.2 to 3.5	–	Congruent LiNbO3 (CLN)	–	–	Volk & Wöhlecke, Springer Series in Materials Science 115 (2009) derived: ratio of the Volk & Wöhlecke 2009 Table 7.1 CLN and SLN values; p. 184 states a factor of three (ref. Chen et al. 2001)	Table 7.1, p. 185; p. 184 ('factor of three', ref. Chen et al. 2001)	C
Differs from Gopalan et al. 1998 (4-5); the sources measured different crystals.

Congruent LiNbO3 (CLN)CLN (C = 0.484) vs near-SLN (C = 0.498)

P(abs)

≈ 4 to 5

T room temperature

Gopalan et al., Applied Physics Letters 72 1981 (1998), abstract

Congruent LiNbO3 (CLN)

3.2 to 3.5

conditions not stated

Differs from Gopalan et al. 1998 (4-5); the sources measured different crystals.

Volk & Wöhlecke, Springer Series in Materials Science 115 (2009), Table 7.1, p. 185; p. 184 ('factor of three', ref. Chen et al. 2001)derived: ratio of the Volk & Wöhlecke 2009 Table 7.1 CLN and SLN values; p. 184 states a factor of three (ref. Chen et al. 2001)

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