<p>The topic of intermittency has drawn a lot of interest lately in the theoretical and experimental study of multiparticle generation. Independent analyses of the intermittent and fractal behavior in emission angle space and azimuthal angle space (i.e., cos<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\theta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>θ</mi> </math></EquationSource> </InlineEquation>-space and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Phi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Φ</mi> </math></EquationSource> </InlineEquation>-space) have been performed for the emission spectra of target-associated fragments from <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(^{84}Kr\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mmultiscripts> <mrow /> <mrow /> <mn>84</mn> </mmultiscripts> <mi>K</mi> <mi>r</mi> </mrow> </math></EquationSource> </InlineEquation>-AgBr interactivity at 1 A GeV. The angular properties of the secondary charged particles can be studied because the nuclear emulsion detector (NED) is a 4<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\pi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>π</mi> </math></EquationSource> </InlineEquation> detector, which allows the measurement of the angles of all emitted charged particles. There is intermittent activity in both areas. The anomaly fractal dimension <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(d_{q}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>d</mi> <mi>q</mi> </msub> </math></EquationSource> </InlineEquation> is determined from the intermittent exponent, and its fluctuation with order q is examined. The aberrant dimension grows with the value of moments q, suggesting a connection between the target-related fragment production process and multifractility.</p>