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ing closer to home, within the confines of the McFadden Act, banks were still endangering the public, which had less of a choice in banking services as a result. The problem with the expansion was that banks were not allowed to own stock in other companies. The prohibition predated the Clayton Act, and was found in the 1864 National Banking Act, but applied to national banks only. The Clayton Act merely extended that prohibition to companies in general. How the acquiring bank structured its deal became important. If it was a bank acting as a bank, then it would be in violation of the act if it had a national charter. But if state banks did the same, a storm would erupt because they could do something national banks could not, reopening the old McFadden issue from the 1920s. Clearly, the way around the problem was to use holding companies. Transamerica did it successfully by being organized specifically to buy the Bank of America. National City was particularly aggressive in New York, using its holding company to expand into the suburbs, something forbidden by state law at the time. Emanuel Celler told New York legislators to stop National City s expansion, which was abhorrent in itself and could start a chain reaction by giant financial institutions in this city that might ultimately wreck the entire banking structure of this state. 4 The idea that big was bad still rang clearly in some quarters in Washington. It was clear from the regulators point of view that the way to control the spread of banks was to restrict the use of holding companies. The purpose-designed shell companies had not been popular since the 1930s and would prove no more popular in the 1950s.

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In Equations (523) and (524), nonlinear gain is included as G t = GN N t N0 1 P t , where = 3 57 10 8 is the nonlinear gain coefficient and P t = E t 2 is the intensity Parameter values are set to realistic values corresponding to a Ga-Al-As semiconductor laser [21, 39] as summarized in Table 51, where Nsol = N0 + 1/ GN p As is common in the field [21, 39], the constant phase shift at the PCM and the detuning parameter were both set to zero, so that the feedback term in Equations (523) and (524) reduces to E t The main bifurcation parameter is the effective feedback strength (a dimensionless parameter), and in two-parameter investigations also the pump current I (in units of ampere) is varied.

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The modelling assumptions here are, as for the LK equations, that the laser operates in single mode and the feedback is weak (because again only a single round trip in the external cavity is taken into account) However, there is the further assumption that the PCM is so fast that the phase-conjugation can be modelled as instantaneous The effect of non-instanteneous PCF has been considered in [4, 26, 59] As the interaction time in the PCM is increased from zero (the instantaneous case), the dynamics of the PCF laser is affected first for larger and then for lower and lower values of For the moderate values of near and just above the locking region (of steady state operation; see Section 552) of the PCF laser used in the results below, the dynamics is essentially unaffected when the interaction time in the PCM does not exceed 0.

1 ns, which appears to be achievable with semiconductor PCMs, see [4] and also 3 The general picture of the dynamics that emerged from earlier studies by numerical simulation is that there are windows where the PCF laser has stable periodic orbits, also called external cavity modes (ECMs) of the PCF laser [1, 21, 39] When the laser operates at an ECM, then it produces periodic output at a frequency that is very close to a multiple of the external round-trip frequency Different ECMs are separated from each other by bubbles of more complicated dynamics, including regions of chaos The transitions through these bubbles can be interpreted as a competition in the laser between neighbouring ECMs, see [21, 39] for more details.