Richard A. Brooker

Richard A. Brooker

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Richard A. Brooker

School of Earth Sciences, University of Bristol, Bristol, UK

Research Focus & Metrics

Academic Career Length

37Years (1990-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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6 January 2016 in Nature
Verified
Journal Article
Closed access
ATAndrew R. Thomson
Andrew R. Thomson
MWMichael J. Walter
Michael J. Walter
SKSimon C. Kohn
Simon C. Kohn
RBRichard A. Brooker
Richard A. Brooker

24 September 2016 in Contributions to Mineralogy and Petrology
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Journal Article
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EME. J. F. Mutch
E. J. F. Mutch
JBJ. D. Blundy
J. D. Blundy
BTB. C. Tattitch
B. C. Tattitch
FCF. J. Cooper
F. J. Cooper
RBR. A. Brooker
R. A. Brooker
We report new experimental data on the composition of magmatic amphiboles synthesised from a variety of granite (sensu lato) bulk compositions at near-solidus temperatures and pressures of 0.8–10 kbar. The total aluminium content (Altot) of the synthetic calcic amphiboles varies systematically with pressure (P), although the relationship is nonlinear at low pressures (<2.5 kbar). At higher pressures, the relationship resembles that of other experimental studies, which suggests of a general relationship between Altot and P that is relatively insensitive to bulk composition. We have developed a new Al-in-hornblende geobarometer that is applicable to granitic rocks with the low-variance mineral assemblage: amphibole + plagioclase (An15–80) + biotite + quartz + alkali feldspar + ilmenite/titanite + magnetite + apatite. Amphibole analyses should be taken from the rims of grains, in contact with plagioclase and in apparent textural equilibrium with the rest of the mineral assemblage at temperatures close to the haplogranite solidus (725 ± 75 °C), as determined from amphibole–plagioclase thermometry. Mean amphibole rim compositions that meet these criteria can then be used to calculate P (in kbar) from Altot (in atoms per formula unit, apfu) according to the expression: $${\textit{P }}\left( {\text{kbar}} \right) = 0.5 + 0.331\left( 8 \right) \times {\text{Al}}^{\text{tot}} + 0.995\left( 4 \right) \times \left( {{\text{Al}}^{\text{tot}} } \right)^{2}$$ This expression recovers equilibration pressures of our calibrant dataset, comprising both new and published experimental and natural data, to within ±16 % relative uncertainty. An uncertainty of 10 % relative for a typical Altot value of 1.5 apfu translates to an uncertainty in pressure estimate of 0.5 kbar, or 15 % relative. Thus the accuracy of the barometer expression is comparable to the precision with which near-solidus amphibole rim composition can be characterised.

1 January 2007 in Geochimica et Cosmochimica Acta
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Journal Article
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AJA.B. Jeffcoate
A.B. Jeffcoate
TET. Elliott
T. Elliott
SKS.A. Kasemann
S.A. Kasemann
DID. Ionov
D. Ionov
KCK. Cooper
K. Cooper
RBR. Brooker
R. Brooker

24 December 2010 in Journal of Petrology
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RBR. A. Brooker
R. A. Brooker
BKB. A. Kjarsgaard
B. A. Kjarsgaard
We present new experiments, combined with a re-evaluation of published data, to characterize the topology of the silicate–carbonate two-liquid solvus in the five-component system SiO2–Na2O–Al2O3–CaO–CO2 (SNAC + CO2). Conjugate liquid compositions have been determined for a wide range of pressures (0·1–2·5 GPa) and temperatures (1225–1700°C) as well as variable degrees of CO2 saturation. The expansion of the two-liquid field with increasing pressure and/or decreasing temperature, and the contraction of the two-liquid field for conditions where PCO2 < Ptotal is accurately presented for the first time. The shape of the two-liquid solvus suggests that alkali-rich carbonatites can have a range of SiO2 + Al2O3 contents down to very low values (<1 wt %), but that low-alkali or alkali-free immiscible carbonatites will always have SiO2 + Al2O3 contents greater than 10–15 wt %. The most commonly observed carbonatite rock compositions observed at the Earth’s surface all tend towards low contents of alkalis SiO2 and Al2O3 and would have fractionated silicate phases from the carbonatite parental melts, possibly associated with alkali loss to coexisting fluids. Our results also show that carbonate liquid exsolution can occur from a CO2-undersaturated (PCO2 < Ptot) silicate melt. Although the expanded high-pressure miscibility gap appears favourable for producing natural silicate melt compositions, a low-pressure (<1·0 GPa) magma chamber in the crust or perhaps in the shallow mantle below a rift provides the most likely environment for immiscibility to arise owing to the lower CO2 demand of the silicate magma. Unusual textures in some experiments, suggestive of a deformable liquid state for the CaCO3 phase, are conclusively shown to be characteristic of a non-quenchable, high-temperature polymorph of solid calcite. Similar calcite globules with this rounded appearance, which are also observed in some nephelinite lavas and mantle xenoliths, must be solid calcite and not immiscible liquids. This is consistent with the high SiO2 + Al2O3 requirement of low-alkali or alkali-free immiscible carbonate liquids.

23 June 2016 in Contributions to Mineralogy and Petrology
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VMVladimir Matjuschkin
Vladimir Matjuschkin
JBJon D. Blundy
Jon D. Blundy
RBRichard A. Brooker
Richard A. Brooker

1 February 2007 in Geochimica et Cosmochimica Acta
Verified
Journal Article
Closed access
VHVeronika S. Heber
Veronika S. Heber
RBRichard A. Brooker
Richard A. Brooker
SKSimon P. Kelley
Simon P. Kelley
BWBernard J. Wood
Bernard J. Wood