Fractals in Higher Dimensions
... insisted. So I am working. Finally, I want to thank my wife Huong, who was very understanding at several times as I was working on this book. It took longer than I expected. I hope it is better because of the delay. ...
... insisted. So I am working. Finally, I want to thank my wife Huong, who was very understanding at several times as I was working on this book. It took longer than I expected. I hope it is better because of the delay. ...
Global exact controllability in infinite time of Schrödinger equation
... when time t goes to infinity. Observing that the linearized system is controllable in infinite time at almost any point, we conclude the controllability of the nonlinear system (in the case d = 1), using an inverse mapping theorem for multivalued functions [21] by Nachi and Penot. Thus (1.1), (1.2) ...
... when time t goes to infinity. Observing that the linearized system is controllable in infinite time at almost any point, we conclude the controllability of the nonlinear system (in the case d = 1), using an inverse mapping theorem for multivalued functions [21] by Nachi and Penot. Thus (1.1), (1.2) ...
FP numbers
... exponent (11-bits), and mantissa (52-bits). • In order to pack more bits into the mantissa the leading 1 to the left of the binary point is implicit. Thus a binary FP number is: (-1)sign*(1 + mantissa)*2exponent • This representation isn't unique to MIPS. It is part of the ...
... exponent (11-bits), and mantissa (52-bits). • In order to pack more bits into the mantissa the leading 1 to the left of the binary point is implicit. Thus a binary FP number is: (-1)sign*(1 + mantissa)*2exponent • This representation isn't unique to MIPS. It is part of the ...
