Layout 1
... as H-Pro-Pro-Asp-NH2 ( 1), H-D-Pro-Pro-Asp-NH2 (2) and H-D-Pro-Pro-Glu-NH2 ( 3) are highly effective ... Layout 1 SYNFORM People, Trends and Views in Synthetic Organic Chemistry 2009/ 01 Thieme Chemistry ... as H-Pro-Pro-Asp-NH2 ( 1), H-D-Pro-Pro-Asp-NH2 (2) and H-D-Pro-Pro-Glu-NH2 ( 3) are highly effective ... Layout 1 ... Layout 1 ...
Folie 1
... ://doi.org/10.1007/s10648-016-9365- 3 Rau, M., Aleven, V., & Rummel, N. (2009). Intelligent Tutoring Systems ... Folie 1 How to Unfold the Potential of Multiple Representations Sarah Malone & Roland Brünken How ... ://doi.org/10.1007/s10648-016-9365- 3 Rau, M., Aleven, V., & Rummel, N. (2009). Intelligent Tutoring Systems ... Folie 1 ... Folie 1 ...
Slide 1
... = 3 → release(barrier) count++ (count= 1) barrier = 0 barrier = 2 barrier = 1 turnstile(barrier ... Slide 1 spcl.inf.ethz.ch @spcl_eth TORSTEN HOEFLER Parallel Programming, Spring 2019, Lecture 16+ 1 ... = 3 → release(barrier) count++ (count= 1) barrier = 0 barrier = 2 barrier = 1 turnstile(barrier ... Slide 1 ... Slide 1 ...
3, 2, 1, … liftoff! – RETHINK
... 3, 2, 1, … liftoff! – RETHINK ... https://blogs.ethz.ch/RETHINK/2019/03/30/ 3-2- 1-liftoff/ ... 3, 2, 1, … liftoff! – RETHINK ...
Slide 1
... 10- 1 100 101 Field frequency (a.u.) 10- 3 10-2 10- 1 100 101 102 103 104 105 106 107 In te n s it y ( a ... is not a plausible index: F= 1 is relativistic at = 10- 3 and nonrelativistic at = 101 10- 3 10-2 10- 1 ... 10- 1 100 101 Field frequency (a.u.) 10- 3 10-2 10- 1 100 101 102 103 104 105 106 107 In te n s it y ( a ... is not a plausible index: F= 1 is relativistic at = 10- 3 and nonrelativistic at = 101 10- 3 10-2 10- 1 ... Slide 1 ...
Slide 1
... . 2 3 10- 3 10-2 10- 1 100 101 Field frequency (a.u.) 10-4 10- 3 10-2 10- 1 100 101 102 103 104 In te n s ... ( ) ( ); ( ) ( ). 2 2 i t i tF t d e f f dte F t In 3 dimensions: 3 3 3 1 ( ( ( (2 ) i iF )= d pe f ); f( )= d re F ... . 2 3 10- 3 10-2 10- 1 100 101 Field frequency (a.u.) 10-4 10- 3 10-2 10- 1 100 101 102 103 104 In te n s ... ( ) ( ); ( ) ( ). 2 2 i t i tF t d e f f dte F t In 3 dimensions: 3 3 3 1 ( ( ( (2 ) i iF )= d pe f ); f( )= d re F ... Slide 1 ...
Diapositivo 1
... carried out. Models Conclusions ERSTA (2008-2011) SHARE (2009-2013) b_value EC8 (2006) 1 2 3 4 5 Períodos ... Lower Tagus Valley 1 2 3 4 5 Zona 7 Zona J Zona 253 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 EC8 ERSTA SHARE a Zona ... carried out. Models Conclusions ERSTA (2008-2011) SHARE (2009-2013) b_value EC8 (2006) 1 2 3 4 5 Períodos ... Lower Tagus Valley 1 2 3 4 5 Zona 7 Zona J Zona 253 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 EC8 ERSTA SHARE a Zona ... Diapositivo 1 ...
Slide 1
... . Bortis F. Krismer 18 Ph.D. Students 1 PostDoc 3 Research Fellows Leading Univ. in Europe Power Electronic ... N I I N 2 3 C,max, 2 ˆ 1 ( ) 32 N O S U f fU N ! ● Scalability / Manufacturability ... . Bortis F. Krismer 18 Ph.D. Students 1 PostDoc 3 Research Fellows Leading Univ. in Europe Power Electronic ... N I I N 2 3 C,max, 2 ˆ 1 ( ) 32 N O S U f fU N ! ● Scalability / Manufacturability ... Slide 1 ...
Slide 1
... confusion with the energy E. 4 5 10- 3 10-2 10- 1 100 101 Field frequency (a.u.) 10- 3 10-2 10- 1 100 101 102 ... .=3.51e16W/cm2F 6 10- 3 10-2 10- 1 100 101 Field frequency (a.u.) 10- 3 10-2 10- 1 100 101 102 103 104 105 106 ... confusion with the energy E. 4 5 10- 3 10-2 10- 1 100 101 Field frequency (a.u.) 10- 3 10-2 10- 1 100 101 102 ... .=3.51e16W/cm2F 6 10- 3 10-2 10- 1 100 101 Field frequency (a.u.) 10- 3 10-2 10- 1 100 101 102 103 104 105 106 ... Slide 1 ...
Diapositive 1
... 1.2 0 1 2 3 4 0 5 10 15 400 K 380 K 360 K 340 K 320 K 300 K Current (A) Vo lta ge ( V ) D385-22 12 µm x ... = 3.25 µm 150°C λ = 3.34 µm 0 1 2 3 4 5 6 0 10 20 30 0.0 0.5 1.0 Current (A) V ol ta ge ( V ) D429-5 HR ... 1.2 0 1 2 3 4 0 5 10 15 400 K 380 K 360 K 340 K 320 K 300 K Current (A) Vo lta ge ( V ) D385-22 12 µm x ... = 3.25 µm 150°C λ = 3.34 µm 0 1 2 3 4 5 6 0 10 20 30 0.0 0.5 1.0 Current (A) V ol ta ge ( V ) D429-5 HR ... Diapositive 1 ...
