Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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2768 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{2}M_{5}$ | 0.5751 | 0.7459 | 0.771 | [M:[0.9677, 1.0323, 0.7004, 0.7651, 0.9677], q:[0.5991, 0.9677], qb:[0.4332, 0.2673], phi:[0.4332]] | [M:[[7], [-7], [3], [-11], [7]], q:[[-6], [7]], qb:[[-1], [4]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}^{4}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$ | ${}\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}$ | -2 | 2*t^2.101 + t^2.295 + 2*t^2.599 + 2*t^2.903 + t^3.401 + 4*t^4.203 + 2*t^4.396 + t^4.59 + 5*t^4.7 + 2*t^4.894 + 4*t^5.004 + 4*t^5.198 + 5*t^5.502 + 3*t^5.806 - 2*t^6. + 6*t^6.304 + t^6.498 + 2*t^6.692 + 6*t^6.802 + t^6.885 + 4*t^6.996 + 7*t^7.106 + 2*t^7.189 + 6*t^7.3 + 4*t^7.493 + 9*t^7.604 + 3*t^7.797 + 6*t^7.907 - t^8.101 - 4*t^8.295 + 12*t^8.405 - 6*t^8.599 + 4*t^8.709 + t^8.793 + 2*t^8.987 - t^4.3/y - t^6.401/y - t^6.595/y - t^6.899/y + (3*t^7.396)/y + (5*t^7.7)/y + (2*t^7.894)/y + (5*t^8.004)/y + (4*t^8.198)/y + (5*t^8.502)/y + t^8.806/y - t^8.89/y - t^4.3*y - t^6.401*y - t^6.595*y - t^6.899*y + 3*t^7.396*y + 5*t^7.7*y + 2*t^7.894*y + 5*t^8.004*y + 4*t^8.198*y + 5*t^8.502*y + t^8.806*y - t^8.89*y | 2*g1^3*t^2.101 + t^2.295/g1^11 + (2*t^2.599)/g1^2 + 2*g1^7*t^2.903 + g1^2*t^3.401 + 4*g1^6*t^4.203 + (2*t^4.396)/g1^8 + t^4.59/g1^22 + 5*g1*t^4.7 + (2*t^4.894)/g1^13 + 4*g1^10*t^5.004 + (4*t^5.198)/g1^4 + 5*g1^5*t^5.502 + 3*g1^14*t^5.806 - 2*t^6. + 6*g1^9*t^6.304 + t^6.498/g1^5 + (2*t^6.692)/g1^19 + 6*g1^4*t^6.802 + t^6.885/g1^33 + (4*t^6.996)/g1^10 + 7*g1^13*t^7.106 + (2*t^7.189)/g1^24 + (6*t^7.3)/g1 + (4*t^7.493)/g1^15 + 9*g1^8*t^7.604 + (3*t^7.797)/g1^6 + 6*g1^17*t^7.907 - g1^3*t^8.101 - (4*t^8.295)/g1^11 + 12*g1^12*t^8.405 - (6*t^8.599)/g1^2 + 4*g1^21*t^8.709 + t^8.793/g1^16 + (2*t^8.987)/g1^30 - t^4.3/(g1*y) - (g1^2*t^6.401)/y - t^6.595/(g1^12*y) - t^6.899/(g1^3*y) + (3*t^7.396)/(g1^8*y) + (5*g1*t^7.7)/y + (2*t^7.894)/(g1^13*y) + (5*g1^10*t^8.004)/y + (4*t^8.198)/(g1^4*y) + (5*g1^5*t^8.502)/y + (g1^14*t^8.806)/y - t^8.89/(g1^23*y) - (t^4.3*y)/g1 - g1^2*t^6.401*y - (t^6.595*y)/g1^12 - (t^6.899*y)/g1^3 + (3*t^7.396*y)/g1^8 + 5*g1*t^7.7*y + (2*t^7.894*y)/g1^13 + 5*g1^10*t^8.004*y + (4*t^8.198*y)/g1^4 + 5*g1^5*t^8.502*y + g1^14*t^8.806*y - (t^8.89*y)/g1^23 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
1767 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ | 0.5734 | 0.743 | 0.7718 | [M:[0.9972, 1.0028, 0.7131, 0.7187], q:[0.5738, 0.9972], qb:[0.429, 0.2841], phi:[0.429]] | 2*t^2.139 + t^2.156 + 2*t^2.574 + t^2.992 + t^3.008 + t^3.426 + 4*t^4.279 + 2*t^4.295 + t^4.312 + 5*t^4.713 + 2*t^4.73 + 2*t^5.131 + 5*t^5.148 + t^5.164 + 3*t^5.565 + 2*t^5.582 + t^5.983 - t^6. - t^4.287/y - t^4.287*y | detail |