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Some of these elements (P, Cl, K, Ti, Cr, and Mn) have no

coronal spectroscopic measurements available. Hence, for

these elements MTOF is in some sense providing the first

"coronal observations", as the solar wind is the interplan-

etary extension of the corona. The MTOF sensor is rou-

tinely measuring isotopic abundance variations for sev-

eral elements (neon, magnesium, silicon, sulfur, argon, cal-

cium, iron, and nickel), some of which have never been

previously observed in the solar wind, in solar energetic

particle (SEP) populations, nor spectroscopically in the sun.

Among the brand new isotopes are those of silicon, sulfur,

calcium, chromium, and nickel. MTOF has presented the

first fine time resolution of solar wind abundance varia-

tions for the elements Cr and Fe, and Fe isotopes.

It is already established that solar wind and suprathermal

(SEP) ion composition, both elemental and charge state,

vary according to the source conditions. The so-called first

ionization potential (FIP) effect, which reflects elemental

fractionation in coronal and solar wind elemental abun-

dances compared to photospheric values for elements with

low FIP's ( < 10 eV ), has been observed using long time

averages for slow and CME-related solar wind. The effect
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solar wind flow type, but some of the current theories can

be distinguished by what they predict for different elements based on different physical constants (e.g., in addition to FIP, there

are theories involving the first ionization time, the ionization diffusion length, etc.). MTOF is making a unique contribution to

this study, both in the number of elements that are observable for the first time by a solar wind experiment and by the time

resolution of measurements. These include pivotal elements such as K, Na, Al, which have extremely low FIP's (< 6 eV), and

S, P, and C which have FIPs in the transitional FIP region (near 10 eV).

Both chromium and iron are low FIP elements. The MTOF has obtained a slow solar wind elemental abundance ratio of 52Cr/

56Fe = 0.015 [!] 0.003. This is similar to photospheric values and indicates that chromium behaves in the same manner as iron in

the FIP fractionation process.

Solar Wind Isotopic Abundances Solar wind isotopic measurements by CELIAS/MTOF are unique. Previous spacecraft mea-

surements have been restricted to helium, and foil measurements from the manned lunar expeditions have given results only for

helium, neon, and argon. The Apollo Foil Experiment indicated significant variations in the helium isotopic composition, but

none were observed in the neon isotopic composition. It is generally assumed that the solar wind gives an unbiased sample of

isotopic composition of the corona, and therefore the photosphere, which in turn is assumed to be representative of the outer

solar convective zone. These compositions should then be close to the primordial composition of the solar nebula.

A strong isotopic fractionation in the solar wind is not expected, although weak effects may be caused by the ion-neutral

separation process that takes place in the upper chromosphere/transition region, and potentially fractionation could result in the

inner corona due to differences in Coulomb drag. The measurements from MTOF are being used to determine whether there are

differences in relative isotopic abundances among different solar wind regimes (CME-related, coronal hole, or slow solar wind)

or for the same type of solar wind, but as a function of solar cycle. Differences between different solar wind regimes or the

absence of such differences can be taken as indicators of the faithfulness of solar wind particles of the solar surface composition.

Solar Wind Charge State Abundances The relative ionization states of ions in the corona depend on the local electron tem-

perature and density, the ions' collisional ionization and radiative and dielectronic recombination rates, and the ions' outflow

velocities. The local coronal density and temperature change with altitude, as observed by UVCS. As the solar wind expands

outward, the coronal electron density decreases to the extent that the solar wind ion expansion time scale is short compared to

the ionization and recombination time scales. The relative ionization states become constant, forever reflective of the condi-

tions at the freezing-in altitude. The solar wind ions maintain their chemical and charge state identity as they continue to
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