PMC:4620161 / 31287-31958 JSONTXT

{"project":"0_colil","denotations":[{"id":"26578853-15110015-358042","span":{"begin":49,"end":53},"obj":"15110015"},{"id":"26578853-19913625-358043","span":{"begin":73,"end":77},"obj":"19913625"}],"text":"And the null hypotheses for L2D (Calhoun et al., 2004; Steffener et al., 2010) are tested with the first two bases, (7a) H0L2D:sgn(α1)(α12+α22)1/2=0, (7b) H0L2D:sgn(α11)(α112+α122)1/2=sgn(α21)(α212+α222)1/2 or with all the three bases, (8a) H0L2D:sgn(α1)(α12+α22+α32)1/2=0, (8b) H0L2D:sgn(α11)(α112+α122+α132)1/2=sgn(α21)                                                                        (α212+α222+α232)1/2, where sgn is the sign function. That is, the L2D for ASM is similar to the L2D for ESM, but using the two or three weights associated with the two or three basis functions in ASM and assigning the sign of the canonical response to the resultant L2-distance."}

{"project":"TEST0","denotations":[{"id":"26578853-49-57-358042","span":{"begin":49,"end":53},"obj":"[\"15110015\"]"},{"id":"26578853-73-81-358043","span":{"begin":73,"end":77},"obj":"[\"19913625\"]"}],"text":"And the null hypotheses for L2D (Calhoun et al., 2004; Steffener et al., 2010) are tested with the first two bases, (7a) H0L2D:sgn(α1)(α12+α22)1/2=0, (7b) H0L2D:sgn(α11)(α112+α122)1/2=sgn(α21)(α212+α222)1/2 or with all the three bases, (8a) H0L2D:sgn(α1)(α12+α22+α32)1/2=0, (8b) H0L2D:sgn(α11)(α112+α122+α132)1/2=sgn(α21)                                                                        (α212+α222+α232)1/2, where sgn is the sign function. That is, the L2D for ASM is similar to the L2D for ESM, but using the two or three weights associated with the two or three basis functions in ASM and assigning the sign of the canonical response to the resultant L2-distance."}

{"project":"2_test","denotations":[{"id":"26578853-15110015-38285031","span":{"begin":49,"end":53},"obj":"15110015"},{"id":"26578853-19913625-38285032","span":{"begin":73,"end":77},"obj":"19913625"}],"text":"And the null hypotheses for L2D (Calhoun et al., 2004; Steffener et al., 2010) are tested with the first two bases, (7a) H0L2D:sgn(α1)(α12+α22)1/2=0, (7b) H0L2D:sgn(α11)(α112+α122)1/2=sgn(α21)(α212+α222)1/2 or with all the three bases, (8a) H0L2D:sgn(α1)(α12+α22+α32)1/2=0, (8b) H0L2D:sgn(α11)(α112+α122+α132)1/2=sgn(α21)                                                                        (α212+α222+α232)1/2, where sgn is the sign function. That is, the L2D for ASM is similar to the L2D for ESM, but using the two or three weights associated with the two or three basis functions in ASM and assigning the sign of the canonical response to the resultant L2-distance."}