Dos Santos Ramalho, R., Helffrich, G., Madeira, J., Cosca, M.,
Thomas, C., Quartau, R., Hipólito, A., Rovere, A., Hearty, P. J., &
Ávila, S. P. (2017). Emergence and evolution of Santa Maria Island
(Azores)—The conundrum of uplifted islands revisited.
Geological
Society of America Bulletin
,
129
(3-4), 372-390.
https://doi.org/10.1130/B31538.1
Peer reviewed version
Link to published version (if available):
10.1130/B31538.1
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The emergence and evolution of Santa Maria Island (Azores) – 1
the conundrum of uplifted islands revisited 2
Ricardo S. Ramalho
1,2
, George Helffrich
3
, José Madeira
4,5
, Michael Cosca
6
, Christine 3
Thomas
7
, Rui Quartau
8,5
, Ana Hipólito
9
, Alessio Rovere
10
, Paul J. Hearty
11
, and Sérgio P. 4
Ávila
12,13
5
1
School of Earth Sciences, University of Bristol, Wills Memorial Building, Queen’s Road, 6
Bristol, BS8 1RJ, UK. 7
2
Lamont-Doherty Earth Observatory at Columbia University, Comer Geochemistry Building, 61 8
Route 9W/ PO box 1000, Palisades, NY-10964-8000, USA. 9
3
Earth-Life Science Institute, Tokyo Institute of Technology, 2-12-1-IE-1 Ookayama, Meguro-10
ku, Tokyo, 152-8550, Japan 11
4
Departamento de Geologia, Faculdade de Ciências, Universidade de Lisboa, 1749-016, 12
Lisboa, Portugal. 13
5
Instituto Dom Luiz, Faculdade de Ciências, Universidade de Lisboa, 1749-016, Lisboa, 14
Portugal. 15
6
U.S. Geological Survey, Denver Federal Center, MS 963, Denver, CO 80225, USA. 16
7
Institut für Geophysik, Westfälische Wilhelms-Universität, Corrensstraße 24, 48149 Münster, 17
Germany 18
8
Divisão de Geologia Marinha, Instituto Hidrográfico, Rua das Trinas, 49, 1249-093 Lisboa, 19
Portugal 20
9
Instituto de Investigação em Vulcanologia e Avaliação de Riscos, Universidade dos Açores, 21
Rua da Mãe de Deus, Edifício do Complexo Científico, 3º Andar - Ala Sul, 9500-321 Ponta 22
Delgada, Açores, Portugal. 23
10
MARUM, University of Bremen and ZMT, Leibniz Center for Tropical Marine Ecology, 24
Marum Pavillion 1110, Bremen, Germany 25
11
Department of Environmental Studies, University of North Carolina Wilmington, NC-28403, 26
USA 27
12
Faculdade de Ciências da Universidade do Porto, Rua do Campo Alegre s/n, 4169-007 Porto, 28
Portugal. 29
13
CIBIO, Centro de Investigação em Biodiversidade e Recursos Genéticos, InBIO Laboratório 30
Associado, Pólo dos Açores, Departamento de Biologia da Universidade dos Açores, Campus de 31
Ponta Delgada, Apartado 1422, 9501-801 Ponta Delgada, Açores, Portugal 32
33
ABSTRACT 34
The growth and decay of ocean island volcanoes is intrinsically linked to vertical 35
movements; whilst the causes for subsidence are well understood, uplift mechanisms remain 36
enigmatic. Santa Maria Island in the Azores Archipelago is an ocean island volcano resting on 37
top of young lithosphere, barely 480 km away from the Mid-Atlantic Ridge. Like most other 38
Azorean islands, Santa Maria should be experiencing subsidence. Yet, several features indicate 39
an uplift trend instead. In this paper we reconstruct the evolutionary history of Santa Maria with 40
respect to the timing and magnitude of its vertical movements, using detailed fieldwork and 41
40
Ar/
39
Ar geochronology. Our investigations revealed a complex evolutionary history spanning 42
~6 Ma, with subsidence followed by uplift extending to the present day. The fact that an island 43
located in young lithosphere experienced such a pronounced uplift trend is remarkable and raises 44
important questions concerning possible uplift mechanisms. Localized uplift in response to the 45
tectonic regime affecting the southeastern tip of the Azores Plateau is unlikely since the area is 46
under transtension. Our analysis shows that the only viable mechanism able to explain the uplift 47
is crustal thickening by basal intrusions, suggesting that intrusive processes play a significant 48
role even on islands standing on young lithosphere, such as in the Azores. 49
50
51
INTRODUCTION 52
Ocean island volcanoes are typically subjected to long-term subsidence, as the linear, 53
age-progressive island chains of the Pacific Ocean clearly exemplify. This subsidence trend is 54
essentially driven by mechanisms such as volcanic surface loading (Moore, 1970; Walcott, 1970; 55
Menard, 1983), plate cooling with age (Parsons and Sclater, 1977; Stein and Stein, 1992), and 56
hotspot swell decay (Morgan et al., 1995), all of which are influenced by fast plate movement 57
away from the melting source. All these mechanisms (with perhaps the exception of hotspot 58
swell decay) are reasonably well understood and are consistent within the plate tectonics/isostasy 59
framework. In a similar fashion, within this fast-moving plate scenario, uplift episodes are easily 60
explained by plate bending due to surface loading of younger islands further “upstream” along 61
the chain (Walcott, 1970; Huppert et al., 2015), or by outer trench rise for islands approaching a 62
subduction zone (Schmidt and Schmincke, 2000). A few island systems (e.g. the Cape Verdes, 63
the Canaries, and Madeira Archipelago), however, fall out of pattern and feature numerous 64
volcanic edifices that experienced pronounced uplift trends, vertical stability, or complex 65
uplift/subsidence histories (e.g. Stautigel and Schmincke, 1984; Klügel et al., 1995; Schmidt and 66
Schmincke, 2002; Menendez et al., 2008; Ramalho et al., 2010a,b,c; Madeira et al., 2010; 67
Sepúlveda et al., 2015; Ramalho et al., 2015). These are mostly concentrated in – but not 68
restricted to – the NE Atlantic, where the Nubian plate moves very slowly or is quasi-stationary 69
with respect to the islands’ melting source (Burke and Wilson, 1972; Ramalho et al., 2010b; 70
Ramalho et al., 2015). The mechanisms behind such uplift trends or episodes, however, are still 71
not completely understood and are the subject of contemporaneous debate, being the focus of the 72
present study. 73
Several plausible mechanisms have been put forward to explain ocean island uplift, all of 74
which are likely to contribute in greater or lesser degree to the observed uplift trends/episodes. 75
For uplift acting at broad regional scale, hotspot swell growth by either spreading of melt residue 76
or dynamic topography is regarded as the most plausible mechanism (Morgan et al., 1995; Zhong 77
and Watts, 2002; Ramalho et al., 2010b; Wilson et al., 2010, Ramalho, 2011). At smaller 78
regional scales uplift may be generated by flexural uplift at the forebulge created by surface 79
loading of nearby younger islands/seamounts (McNutt and Menard, 1978; Watts and ten Brink, 80
1989; Grigg and Jones, 1997; Huppert et al., 2015), by flexural uplift induced by subsurface 81
loads (“underplating”)(Watts and ten Brink, 1989; Ali et al., 2003), or by flexural rebound driven 82
by mass wasting or erosion (Menard, 1983; Smith and Wessel, 2000; Menendez et al., 2008). 83
However, these uplift mechanisms still act upon a wide area (which largely depends on plate 84
rheology) and thus cannot be accounted to explain contrasting uplift histories for edifices 85
spatially close together (Ramalho et al., 2010a,b,c). Additionally, surface loading has been 86
shown to only generate uplift in the order of 10’s of meters (unless unrealistically thin elastic 87
thicknesses are considered)(McNutt and Menard, 1978). It also requires younger edifices being 88
loaded at a suitable distance, and fails to explain long-term uplift trends. In a similar fashion, 89