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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8458 | Sp2adj1nf1 | $\phi_1^2X_1$ + $ \phi_1^8$ + $ q_1q_2X_2$ + $ M_1\phi_1^3q_1q_2$ + $ M_2\phi_1q_1^2$ | 0.9818 | 1.1393 | 0.8618 | [X:[1.5, 1.5], M:[0.75, 1.2307], q:[0.2596, 0.2404], qb:[], phi:[0.25]] | [X:[[0], [0]], M:[[0], [2]], q:[[-1], [1]], qb:[], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
$\phi_1q_2^2$, $ M_1$, $ \phi_1q_1q_2$, $ \phi_1^4$, $ \phi_1^2q_1q_2$, $ M_2$, $ \phi_1^3q_2^2$, $ \phi_1^3q_1^2$, $ \phi_1^2q_2^4$, $ M_1\phi_1q_2^2$, $ \phi_1^2q_1q_2^3$, $ M_1^2$, $ M_1\phi_1q_1q_2$, $ \phi_1^2q_1^2q_2^2$, $ X_1$, $ X_2$, $ \phi_1^5q_2^2$, $ \phi_1^3q_1q_2^3$, $ M_1\phi_1^4$, $ M_1\phi_1^2q_1q_2$, $ \phi_1^5q_1q_2$, $ \phi_1^3q_1^2q_2^2$, $ M_2\phi_1q_2^2$, $ \phi_1^4q_2^4$, $ M_1M_2$, $ M_2\phi_1q_1q_2$, $ M_1\phi_1^3q_2^2$, $ \phi_1^4q_1q_2^3$ | $\phi_1^6q_1q_2$, $ \phi_1^4q_1^2q_2^2$ | 1 | t^2.19+2*t^2.25+2*t^3.+2*t^3.69+t^3.81+t^4.38+2*t^4.44+5*t^4.5+2*t^5.19+4*t^5.25+2*t^5.88+3*t^5.94+t^6.+t^6.06+t^6.58+2*t^6.63+7*t^6.69+6*t^6.75+5*t^7.38+3*t^7.44+9*t^7.5-t^7.56+t^7.62+2*t^8.08+3*t^8.13+7*t^8.19-t^8.25+t^8.31+t^8.77+2*t^8.83+7*t^8.88+6*t^8.94-t^8.94/y^2-t^3.75/y-t^5.25/y-t^5.94/y-(2*t^6.)/y-t^6.75/y-t^8.13/y+(2*t^8.88)/y+(2*t^8.94)/y-t^3.75*y-t^5.25*y-t^5.94*y-2*t^6.*y-t^6.75*y-t^8.13*y+2*t^8.88*y+2*t^8.94*y-t^8.94*y^2 | g1^2*t^2.19+2*t^2.25+2*t^3.+2*g1^2*t^3.69+t^3.81/g1^2+g1^4*t^4.38+2*g1^2*t^4.44+5*t^4.5+2*g1^2*t^5.19+4*t^5.25+2*g1^4*t^5.88+3*g1^2*t^5.94+t^6.+t^6.06/g1^2+g1^6*t^6.58+2*g1^4*t^6.63+7*g1^2*t^6.69+6*t^6.75+5*g1^4*t^7.38+3*g1^2*t^7.44+9*t^7.5-t^7.56/g1^2+t^7.62/g1^4+2*g1^6*t^8.08+3*g1^4*t^8.13+7*g1^2*t^8.19-t^8.25+t^8.31/g1^2+g1^8*t^8.77+2*g1^6*t^8.83+7*g1^4*t^8.88+6*g1^2*t^8.94-(g1^2*t^8.94)/y^2-t^3.75/y-t^5.25/y-(g1^2*t^5.94)/y-(2*t^6.)/y-t^6.75/y-(g1^4*t^8.13)/y+(2*g1^4*t^8.88)/y+(2*g1^2*t^8.94)/y-t^3.75*y-t^5.25*y-g1^2*t^5.94*y-2*t^6.*y-t^6.75*y-g1^4*t^8.13*y+2*g1^4*t^8.88*y+2*g1^2*t^8.94*y-g1^2*t^8.94*y^2 |
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 |
---|---|---|---|---|---|---|---|---|---|
8221 | Sp2adj1nf1 | $\phi_1^2X_1$ + $ \phi_1^8$ + $ q_1q_2X_2$ + $ M_1\phi_1^3q_1q_2$ | 1.0005 | 1.1724 | 0.8534 | [X:[1.5, 1.5], M:[0.75], q:[0.25, 0.25], qb:[], phi:[0.25]] | 4*t^2.25+2*t^3.+2*t^3.75+12*t^4.5+8*t^5.25+6*t^6.-t^3.75/y-t^5.25/y-(4*t^6.)/y-t^3.75*y-t^5.25*y-4*t^6.*y | detail | {a: 2049/2048, c: 2401/2048, X1: 3/2, X2: 3/2, M1: 3/4, q1: 1/4, q2: 1/4, phi1: 1/4} |