INSTITUTO POLITÉCNICO NACIONAL - Instituto Avanzado de ...

6. SOLUCIÓN PARA LA TEORÍA EMDA PARA SUBESPACIOS 1-DIMENSIONALES 115mientras que la carga dilatónica Q D está dada porQ D =m 0m 0 (B 2 +(2m 0 e 2pm 0 2e pm 0 )B+2m 2 0 e4pm 0 2m 0 e 3pm 0 +e 2pm 0 )[ e pm 0B 3 + (3 + (p 2e pm 0)m 0 )B 2+( 2e 2pm 0pm 2 0 + (4e 2pm 02pe pm 0)m 0 3e pm 0)B4e 4pm 0pm 3 0 + 2e 3pm 0pm 2 0 + ( 2e 3pm 0+ e 2pm 0p)m 0 + e 2pm 0]; (6.30)…nalmente, la carga axiónica Q a esQ a =4m 2 0 m 0e pm 0(e 2pm 0 B 4 4e 3pm 0 B 3 +(6e 4pm 0 +2m 2 0 )B2 +( 4e 5pm 0 4m 2 0 epm 0 )B+2(m 2 0 +1)e2pm 0 m 2 0 +e6pm 0 ) 2[B 6 e pm 0p + (m 0 6p)e 2pm 0B 5 + (15p 5m 0 + m 2 0p)e 3pm 0B 4+((10m 0 20p 4m 2 0p)e 4pm 0+ m 3 0)B 3+((6m 2 0p 10m 0 + 15p)e 5pm 0(m 0 p + 3)m 3 0e pm 0)B 2+( (6p 4m 2 0p 5m 0 )e 6pm 0+ (3 + 2m 0 p)m 3 0e 2pm 0)B+(e 7pm 0pm 2 0 + p m 0 )e 7pm 0(1 + pm 0 )m 3 0e 3pm 0]: (6.31)