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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1621 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{7}$ | 0.6729 | 0.8357 | 0.8052 | [M:[1.1628, 1.1162, 0.9304, 1.0, 0.8372, 0.7209, 0.8372], q:[0.7791, 0.4534], qb:[0.3838, 0.6162], phi:[0.4419]] | [M:[[-3], [4], [-11], [0], [3], [-1], [3]], q:[[1], [7]], qb:[[-4], [4]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{6}$, ${ }M_{5}$, ${ }M_{7}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{3}M_{6}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{5}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{7}$, ${ }M_{6}q_{1}q_{2}$ | ${}$ | -2 | t^2.163 + 2*t^2.511 + t^2.791 + t^3. + t^3.349 + t^3.628 + t^3.697 + t^4.046 + t^4.186 + 2*t^4.326 + t^4.534 + 2*t^4.674 + t^4.954 + 4*t^5.023 + t^5.163 + t^5.303 + 2*t^5.511 + t^5.583 + t^5.791 + 3*t^5.86 - 2*t^6. + 2*t^6.14 + 2*t^6.209 + t^6.349 + t^6.42 + t^6.489 + 2*t^6.557 + 3*t^6.697 + 2*t^6.837 + 3*t^7.046 + t^7.117 + 3*t^7.186 + t^7.257 + t^7.326 + t^7.394 + t^7.466 + 5*t^7.534 + 2*t^7.674 + t^7.743 + t^7.746 + t^7.814 + t^7.883 + 2*t^7.954 + 3*t^8.023 + t^8.092 + t^8.094 - 3*t^8.163 + t^8.232 + t^8.303 + 5*t^8.372 + t^8.374 - 4*t^8.511 + t^8.58 + t^8.583 + 4*t^8.651 + 4*t^8.72 - 2*t^8.791 + t^8.86 + t^8.931 - t^4.326/y - t^6.489/y - t^6.837/y - t^7.117/y + t^7.534/y + (2*t^7.674)/y + t^7.814/y + t^7.954/y + t^8.023/y + (2*t^8.163)/y + (2*t^8.303)/y + (3*t^8.511)/y - t^8.651/y + (2*t^8.791)/y + (3*t^8.86)/y - t^4.326*y - t^6.489*y - t^6.837*y - t^7.117*y + t^7.534*y + 2*t^7.674*y + t^7.814*y + t^7.954*y + t^8.023*y + 2*t^8.163*y + 2*t^8.303*y + 3*t^8.511*y - t^8.651*y + 2*t^8.791*y + 3*t^8.86*y | t^2.163/g1 + 2*g1^3*t^2.511 + t^2.791/g1^11 + t^3. + g1^4*t^3.349 + t^3.628/g1^10 + g1^8*t^3.697 + g1^12*t^4.046 + g1^5*t^4.186 + (2*t^4.326)/g1^2 + g1^9*t^4.534 + 2*g1^2*t^4.674 + t^4.954/g1^12 + 4*g1^6*t^5.023 + t^5.163/g1 + t^5.303/g1^8 + 2*g1^3*t^5.511 + t^5.583/g1^22 + t^5.791/g1^11 + 3*g1^7*t^5.86 - 2*t^6. + (2*t^6.14)/g1^7 + 2*g1^11*t^6.209 + g1^4*t^6.349 + t^6.42/g1^21 + t^6.489/g1^3 + 2*g1^15*t^6.557 + 3*g1^8*t^6.697 + 2*g1*t^6.837 + 3*g1^12*t^7.046 + t^7.117/g1^13 + 3*g1^5*t^7.186 + t^7.257/g1^20 + t^7.326/g1^2 + g1^16*t^7.394 + t^7.466/g1^9 + 5*g1^9*t^7.534 + 2*g1^2*t^7.674 + g1^20*t^7.743 + t^7.746/g1^23 + t^7.814/g1^5 + g1^13*t^7.883 + (2*t^7.954)/g1^12 + 3*g1^6*t^8.023 + g1^24*t^8.092 + t^8.094/g1^19 - (3*t^8.163)/g1 + g1^17*t^8.232 + t^8.303/g1^8 + 5*g1^10*t^8.372 + t^8.374/g1^33 - 4*g1^3*t^8.511 + g1^21*t^8.58 + t^8.583/g1^22 + (4*t^8.651)/g1^4 + 4*g1^14*t^8.72 - (2*t^8.791)/g1^11 + g1^7*t^8.86 + t^8.931/g1^18 - t^4.326/(g1^2*y) - t^6.489/(g1^3*y) - (g1*t^6.837)/y - t^7.117/(g1^13*y) + (g1^9*t^7.534)/y + (2*g1^2*t^7.674)/y + t^7.814/(g1^5*y) + t^7.954/(g1^12*y) + (g1^6*t^8.023)/y + (2*t^8.163)/(g1*y) + (2*t^8.303)/(g1^8*y) + (3*g1^3*t^8.511)/y - t^8.651/(g1^4*y) + (2*t^8.791)/(g1^11*y) + (3*g1^7*t^8.86)/y - (t^4.326*y)/g1^2 - (t^6.489*y)/g1^3 - g1*t^6.837*y - (t^7.117*y)/g1^13 + g1^9*t^7.534*y + 2*g1^2*t^7.674*y + (t^7.814*y)/g1^5 + (t^7.954*y)/g1^12 + g1^6*t^8.023*y + (2*t^8.163*y)/g1 + (2*t^8.303*y)/g1^8 + 3*g1^3*t^8.511*y - (t^8.651*y)/g1^4 + (2*t^8.791*y)/g1^11 + 3*g1^7*t^8.86*y |
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 |
---|---|---|---|---|---|---|---|---|---|
1038 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}q_{2}\tilde{q}_{2}$ + ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.659 | 0.8115 | 0.8121 | [M:[1.159, 1.1213, 0.9165, 1.0, 0.841, 0.7197], q:[0.7803, 0.4622], qb:[0.3787, 0.6213], phi:[0.4394]] | t^2.159 + t^2.523 + t^2.749 + t^3. + t^3.364 + t^3.477 + t^3.59 + t^3.728 + t^4.092 + t^4.205 + 2*t^4.318 + t^4.569 + t^4.682 + t^4.908 + 2*t^5.046 + t^5.159 + t^5.499 + t^5.523 + t^5.636 + t^5.749 + 2*t^5.887 - t^6. - t^4.318/y - t^4.318*y | detail |