The Galactic center H II region, G0.18-0.04, also known as the ''Sickl
e,'' is located where the nonthermal ''Arc'' crosses the Galactic plan
e. The Sickle appears to be the ionized edge of a dense molecular clou
d. The source of ionization has been ascribed to both the interaction
of the cloud with the magnetic field of the Are and to the hot stars i
n the adjacent cluster, AFGL 2004, also known as the ''Quintuplet Clus
ter.'' This paper addresses the relative locations of the stars, the i
onized and molecular gas, and the sources of gas excitation and dust h
eating. The far-infrared forbidden lines of [S III] 18.7 and 33.5 mu m
, [Si II] 34.8 mu m, [Ne III] 36.0 mu m, [O III] 51.8 and 88.4 mu m, [
N III] 57.3 mu m, [O I] 63.2 and 146 mu m, [C II] 158 mu m, and [N II]
205 mu m and the adjacent continua were observed with NASA's Kuiper A
irborne Observatory at 11 positions around G0.18-0.04, including G0.15
-0.05, also known as the ''Pistol.'' The beam size was 40 ''-60 ''. Th
e electron density, the ionic abundances, and the ionization structure
of the H II region were estimated from the doubly ionized line fluxes
. The density and radiation held found in the photodissociation region
(PDR) between the H II region and the molecular cloud were estimated
from the [C II] and [O I] line fluxes and the far-infrared continuum.
The ionization structure and the PDR properties were compared to shell
models of H II regions with varying distances from their exciting sta
rs. The agreement of observations and models indicates that the hot st
ars of AFGL 2004 are the likely source of ionization of the Sickle. Ad
ditional hot stars are necessary to ionize the more outlying positions
. However, the low ionization and high PDR radiation field of the Pist
ol imply that it cannot be as close to AFGL 2004 as is indicated by it
s proximity on the sky. Instead, the Pistol is probably ionized by the
luminous blue variable candidate, Pistol Source A. The extinction to
the region was estimated from the IRAS low-resolution spectrum of AFGL
2004 and from the distribution of the J, H, and K' magnitudes of prev
iously observed stars in the held. The extinction is fairly uniform, w
ith no apparent enhancement due to the molecular clouds. The strength
of Brackett gamma, the 19 mu m lines and continuum, and the IRAS 25 mu
m continuum are all consistent with the absence of a dense, foregroun
d molecular cloud. We conclude that the H II region is on the near sid
e of the dense cloud.