Cataclasis relicta en los mármoles de alta presión del complejo de Samaná, Noreste de la República Dominicana

  1. I. Rodriguez 4
  2. F. J. Fernández 1
  3. J. Escuder-Viruete 2
  4. A. Pérez-Estaún 3
  1. 1 Universidad de Oviedo
    info

    Universidad de Oviedo

    Oviedo, España

    ROR https://ror.org/006gksa02

  2. 2 Instituto Geológico y Minero de España
    info

    Instituto Geológico y Minero de España

    Madrid, España

    ROR https://ror.org/04cadha73

  3. 3 Instituto de Ciencias de la Tierra Jaume Almera
    info

    Instituto de Ciencias de la Tierra Jaume Almera

    Barcelona, España

    ROR https://ror.org/01nsd7y51

  4. 4 Universidad de León
    info

    Universidad de León

    León, España

    ROR https://ror.org/02tzt0b78

Revista:
Boletín geológico y minero

ISSN: 0366-0176

Año de publicación: 2017

Volumen: 128

Número: 3

Páginas: 569-586

Tipo: Artículo

DOI: 10.21701/BOLGEOMIN.128.3.003 DIALNET GOOGLE SCHOLAR

Otras publicaciones en: Boletín geológico y minero

Objetivos de desarrollo sostenible

Resumen

Cold-cathodoluminiscence (CCL) images have unmasked relict cataclastic microstructures in marbles and calc-schists of the higher-pressure units of the Samaná complex. The grain size of the cataclastic microstructures always has a self-similar distribution of power law type, with a slope break at log (ri)=1.7. The large grain size fraction (1.7<log (ri)<2.4) is characterized by fractal dimension D2=2.43 in the calcite-microstructures of the Punta Balandra unit and D2=2.72 in the Santa Bárbara unit. Both D-values are within the usual range of the carbonate-cataclasites and they are significant with the linear correlation of R2 =0.95 and 0.93, respectively. However, the finer grain size fraction (0.9<log (ri)<1.7) is characterized by D1<1 and this grain-size distribution is beyond the fractal-range for pure cataclastic-fabric, even though it has better fit power-law distribution. Microstructures such as dissolution-surfaces, interpenetrated particles and the higher roundness and lower irregularity of the boundary grain from fine fraction indicate that dissolution-precipitation creep was dominant after cataclasis. Clast size and stress reduction after cataclasis and the high fluid pressure provided favourable conditions to allow dissolution-precipitation creep. Transition from cataclastic flow to dissolution-precipitation creep was scale-dependent and it tended to homogenize and reduce the finer grain size fraction. Consequently, the slope break between D1 and D2 is interpreted as a record in the grain size distribution produced by a change in the dominant deformation mechanism.