997 resultados para Carta CUSUM-ln(S2)
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še-ʿiṭṭēr lākem ... Yaʿaqôv Ben- ... Yiṣḥāq ... mim-mišpaḥat rabbēnû ... be-q"q Yānôw
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še-ʿiṭṭēr lākem ... Yaʿaqôv Ben- ... Yiṣḥāq ... mim-mišpaḥat rabbēnû ... be-q"q Yānôw
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še-ʿiṭṭēr lākem ... Yaʿaqôv Ben- ... Yiṣḥāq ... mim-mišpaḥat rabbēnû ... be-q"q Yānôw
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ʿal yedê Yiṣḥāq Ben-Aryê Yôsēf Dōv ...
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še-ʿiṭṭēr lākem ... Yaʿaqôv Ben- ... Yiṣḥāq ... mim-mišpaḥat rabbēnû ... be-q"q Yānôw
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še-ʿiṭṭēr lākem ... Yaʿaqôv Ben- ... Yiṣḥāq ... mi-... Yānôw
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ḥibbērô ... Yiṣḥāq Abôhab
Ḥamiššā ḥūmšê Tôrā ʿim megillôt we-hafṭārôt bi-lšôn aškenaz : ṣe'ênā û-re'ênā benôt Ṣiyyôn bā-ʿaṭārā
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še-ʿiṭṭēr lākem ... Yaʿaqôv Ben- ... Yiṣḥāq ... mi-... Yānôw
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še ʿiṭṭēr lākem ... Yaʿaqôv Ben- ... Yiṣḥāq ... mim-mišpaḥat rabbēnû ... be-q"q Yānôw
Resumo:
še-ʿiṭṭēr lākem ... Yaʿaqôv Ben- ... Yiṣḥāq ... mim-mišpaḥat rabbēnû ... be-q"q Yānôw
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[Jakob Ben-Isaak Aschkenasi]
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še-ʿiṭṭēr lākem ... Yaʿaqôv Ben- ... Yiṣḥāq ...
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We observe the weak S 0 → S 2 transitions of the T-shaped benzene dimers (Bz)2 and (Bz-d 6)2 about 250 cm−1 and 220 cm−1 above their respective S 0 → S 1 electronic origins using two-color resonant two-photon ionization spectroscopy. Spin-component scaled (SCS) second-order approximate coupled-cluster (CC2) calculations predict that for the tipped T-shaped geometry, the S 0 → S 2 electronic oscillator strength f el (S 2) is ∼10 times smaller than f el (S 1) and the S 2 state lies ∼240 cm−1 above S 1, in excellent agreement with experiment. The S 0 → S 1 (ππ ∗) transition is mainly localized on the “stem” benzene, with a minor stem → cap charge-transfer contribution; the S 0 → S 2 transition is mainly localized on the “cap” benzene. The orbitals, electronic oscillator strengths f el (S 1) and f el (S 2), and transition frequencies depend strongly on the tipping angle ω between the two Bz moieties. The SCS-CC2 calculated S 1 and S 2 excitation energies at different T-shaped, stacked-parallel and parallel-displaced stationary points of the (Bz)2 ground-state surface allow to construct approximate S 1 and S 2 potential energy surfaces and reveal their relation to the “excimer” states at the stacked-parallel geometry. The f el (S 1) and f el (S 2) transition dipole moments at the C 2v -symmetric T-shape, parallel-displaced and stacked-parallel geometries are either zero or ∼10 times smaller than at the tipped T-shaped geometry. This unusual property of the S 0 → S 1 and S 0 → S 2 transition-dipole moment surfaces of (Bz)2 restricts its observation by electronic spectroscopy to the tipped and tilted T-shaped geometries; the other ground-state geometries are impossible or extremely difficult to observe. The S 0 → S 1/S 2 spectra of (Bz)2 are compared to those of imidazole ⋅ (Bz)2, which has a rigid triangular structure with a tilted (Bz)2 subunit. The S 0 → S 1/ S 2 transitions of imidazole-(benzene)2 lie at similar energies as those of (Bz)2, confirming our assignment of the (Bz)2 S 0 → S 2 transition.
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BACKGROUND Pemphigus encompasses a group of life-threatening autoimmune bullous diseases characterized by blisters and erosions of the mucous membranes and skin. Before the era of immunosuppressive treatment, the prognosis of pemphigus was almost fatal. Due to its rarity, only few prospective controlled therapeutic trials are available. OBJECTIVES For this reason, a group of European dermatologists with a long-standing interest and expertise in basic and clinical pemphigus research has sought to define diagnostic and therapeutic guidelines for the management of patients with pemphigus. RESULTS This group identified the statements of major agreement or disagreement regarding the diagnostic and therapeutic management of pemphigus. The revised final version of the pemphigus guideline was finally passed on to the European Dermatology Forum (EDF) for a final consensus with the European Academy of Dermatology and Venereology (EADV) and the European Union of Medical Specialists (UEMS).