By William Stolzenburg

ISBN-10: 1620405547

ISBN-13: 9781620405543

Overdue one June evening in 2011, a wide animal collided with an SUV cruising down a Connecticut expressway. The creature seemed as whatever out of recent England's forgotten earlier. Beside the line lay a 140-pound mountain lion.

Speculations ran wild, the wildest of which figured him a ghostly survivor from a bygone century while lions final roamed the japanese usa. yet a extra outstanding state of affairs of proof quickly opened up. The lion used to be 3 years previous, with a DNA path embarking from the Black Hills of South Dakota on a cross-country odyssey finally passing inside of thirty miles of latest York urban. It was once the farthest landbound trek ever recorded for a wild animal in the US, by means of a slightly weaned youngster venturing solo via opposed terrain.

William Stolzenburg retraces his two-year journey--from his embattled birthplace within the Black Hills, around the nice Plains and the Mississippi River, via Midwest metropolises and distant northern forests, to his tragic finale upon Connecticut's Gold Coast. alongside the best way, the lion traverses lands with humans gunning for his type, in addition to these championing his reason.

Heart of a Lion is a narrative of 1 heroic creature pitting intuition opposed to towering odds, coming domestic to a society deeply divided over his go back. It is a testomony to the resilience of nature, and a try of humanity's willingness to stay back beside the final word image of wildness.

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Extra resources for Heart of a Lion: A Lone Cat's Walk Across America

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3) It is assumed that all photoionization events occur at the same distance l from the acceleration region, and that the initial velocity along the flight tube axis is zero. The total TOF is dependent on the mass to charge ratio m/z, and the cations are therefore separated into bunches when they reach the detector with the lightest first followed by successively heavier masses (assuming identical charges). 4) m/z = K ion (tion where all the spectrometer dependent parameters are collected into a single constant K ion , and t0 measures the difference between the laser trigger and the time of photoionization.

Instrum. 26, 1150–1157 (1955) 7. F. Chandezon, B. Huber, C. Ristori, Rev. Sci. Instrum. 65, 3344–3353 (1994) Chapter 3 Fitting of Experimental Data and Cross-Correlation The time-dependent spectra obtained by the procedures described in the previous chapter provide a wealth of information on the dynamical processes of the molecules investigated. To derive manageable data from the spectra, it is often assumed that the individual dynamical steps investigated follow first-order kinetics [1]. In the experiments, the time-resolution is limited by the instrument response function which is dominated by the temporal cross-correlation (XC) between the pump and probe pulses.

Another option is to use a time-dependent DVR with corrections, the so-called correlation DVR, but this approach will not be discussed further, and the reader is referred to Refs. [29] and [30] for further details. The restriction on the form of the Hamiltonian in Eq. 12 implies that one has to chose an appropriate coordinate system. One choice is rectilinear Cartesian coordinates, however, these are often not the most chemically and physically intuitive set of coordinates. In Cartesian coordinates, the kinetic energy operator is diagonal in the nuclear degrees of freedom and, thus, of the form of Eq.

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Heart of a Lion: A Lone Cat's Walk Across America by William Stolzenburg


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