The Effect of Finite Flux Rise Time on Recording Performance

IEEE Transactions on Magnetics

Volumn 6, Issue 1, 1970, Pages 95-100

  Lee, John E ^a   Truman, Norman N ^a  

^a Computer Research and Advanced Development Division International Computers Ltd ^*  (United Kingdom)

Author keywords

[No Author keywords available]

Indexed keywords

CES; COMPUTERS; MEMORIES; RECORDING HEADS;

EID: 0014747083     PISSN: 00189464     EISSN: 19410069     Source Type: Journal    
DOI: 10.1109/TMAG.1970.1066679     Document Type: Article

References (10)

1. P. I. Bonyhard, A. V. Davies, and B. K. Middleton, “A theory of digital magnetic recording on metallic films,” IEEE Trans. Magnetics, vol. MAG-2, pp. 1–5, March 1966.
2. I. Stein, “Generalized pulse recording,” IEEE Trans. Electronic Computers, vol. EC-12, pp. 77–92, April 1963.
3. J. R. Herbert, “A computer simulation of the magnetic recording process,” Proc. 1965 INTERMAG Conf. (Washington, D.C.), pp. 15-1-1-15-1-8.
4. B. Kostyshyn, “A theoretical model for a quantitative evaluation of magnetic recording systems,” IEEE Trans. Magnetics, vol. MAG-2, pp. 236–242, September 1966.
5. J. J. Miyata and R. R. Hartel, “The recording and reproduction of signals on magnetic medium using saturation-type recording,” IRE Trans. Electronic Computers, vol. EC-8, pp. 159–169, June 1959.
6. J. E. Lee and N. N. Truman, “The effect of vertical head field component on the switching of thin metallic films,” IEEE Trans. Magnetics, vol. MAG-4, pp. 277–280, September 1968.
7. L. E. Fay, “Two dimensional theory of the recording head,” Internatl. Conf. on Magnetic Recording, pp. 71–77, July 1969.
8. S. Duinker, “On the resolving power in the process of magnetic recording,” Tijdchr. Ned. Radiogen., vol. 22, pp. 29–48, January 1957.
9. A. V. Davies, “Effects of the writing process and crosstalk on the timing accuracy of pulses in NRZ digital recording,” IEEE Trans. Magnetics, vol. MAG-3, pp. 217–222, September 1967.
10. A. S. Hoagland, Digital Magnetic Recording, 1st ed. New York: Wiley, pp. 120–122.