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Integer data types comprise the following primitive data types: int, long, byte, and short (see Section 22, p 28) The default data type of an integer literal is always int, but it can be specified as long by appending the suffix L (or l) to the integer value Without the suffix, the long literals 2000L and 0l will be interpreted as int literals There is no direct way to specify a short or a byte literal In addition to the decimal number system, integer literals can also be specified in octal (base 8) and hexadecimal (base 16) number systems Octal and hexadecimal numbers are specified with a 0 and 0x (or 0X) prefix respectively Examples of decimal, octal and hexadecimal literals are shown in Table 25 Note that the leading 0 (zero) digit is not the uppercase letter O The hexadecimal digits from a to f can also be specified with the corresponding uppercase forms (A to F) Negative integers (eg -90) can be specified by prefixing the minus sign (-) to the magnitude of the integer regardless of number system (eg, -0132 or -0X5A) Number systems and number representation are discussed in Appendix G Java does not support literals in binary notation

inherited by the class OuterB from its superclass OuterA Thus, an object of class OuterB can act as an outer object for an instance of class InnerA The object creation expression at (9)

0 e B (z)/2

new OuterB()new InnerB();

creates an OuterB object and implicitly passes its reference to the default constructor of class InnerB The default constructor of class InnerB invokes the default constructor of its superclass InnerA by calling super() and passing it the reference of the OuterB object, which the superclass constructor can readily bind to

C (z) 1

class OuterA { // (1) class InnerA { } // (2) } //_____________________________________________________________________________ class SubclassC extends OuterAInnerA { // (3) Extends NSMC at (2) // (4) Mandatory non-default constructor: SubclassC(OuterA outerRef) { outerRefsuper(); }

A simple identi cation gives A(z) = z, e B (z)/2 = cosh | | = (1 |z|2 ) 1/2 , and C (z) = We thus recover in the action (859) of D (z) the SU (1, 1) coherent states (88) z This kind of disentangling technique for factorizing elaborate representation operators is well known [9], and we will use it again in the chapters devoted to squeezed states and to fermionic coherent states

} //_____________________________________________________________________________ class OuterB extends OuterA { // (6) Extends class at (1) class InnerB extends OuterBInnerA { } // (7) Extends NSMC at (2) } //_____________________________________________________________________________ public class Extending { public static void main(String[] args) { // (8) Outer instance passed explicitly in constructor call: new SubclassC(new OuterA()); // (9) No outer instance passed explicitly in constructor call to InnerB: new OuterB()new InnerB(); } }

public class MyClass { public static void main(String[] args) { Outer objRef = new Outer(); Systemoutprintln(objRefcreateInner()getSecret()); } }

Now the new net to the equity investor is:

The inner product (837) vanishes identically at the limit value = 1/2 However, there exists a well-de ned unitary irreducible representation of SU (1, 1) corresponding to this value Its carrier space can be realized as the Hilbert space L2 (S 1 , d /2 ) of the exponential Fourier series, that is, the space of square-integrable complex-valued functions on the boundary S 1 of the unit disk D Indeed, the action (829) of g= SU (1, 1)

368 class Outer { private int secret; Outer() { secret = 123; } class Inner { int getSecret() { return secret; } }

Inner createInner() { return new Inner(); } }

on D extends to the boundary as g e i = ( e i + ) ( e i + ) 1 = e i S 1 , (860)